Practical Guide to Free-Energy Devices

From: Subject: Practical Guide to Free-Energy Devices - Chapter 8 Date: Sun, 28 Mar 2010 16:29:48 +0200 MIME-Version: 1.0 Content-Type: multipart/related; type="text/html"; boundary="----=_NextPart_000_0000_01CACE93.E2558410" X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2900.5579 This is a multi-part message in MIME format. ------=_NextPart_000_0000_01CACE93.E2558410 Content-Type: text/html; charset="Windows-1252" Content-Transfer-Encoding: quoted-printable Content-Location: http://free-energy-info.co.uk/Chapt8.html Practical Guide to Free-Energy Devices - Chapter = 8
A Practical Guide to = Free-Energy=20 = Devices = &= nbsp; =20 = &= nbsp; &n= bsp; &nb= sp; Auth= or:=20 Patrick J. Kelly

Chapter 8:=20 Self-Powered Engines

We have been raised = with the idea=20 that it is necessary to burn a fuel to produce power which we can = use.=20 We are sold coal, coke, timber, paraffin/kerosene, = petrol/gasoline,=20 diesel, propane, etc. for us to burn in order to =93get=94 energy. = =20 While it is perfectly true that burning these things will indeed = result in=20 energy in a form which we find convenient to use in heating, = cooling,=20 powering engines, etc. what is carefully avoided is the fact that = it is=20 not at all necessary to burn a fuel in order to run the things = which we=20 want to power. This =91inconvenient=92 fact has been = concealed and=20 denied for more than fifty years now (very surprisingly, by the = people who=20 want to sell us these fuels to burn =96 do you perhaps think that = they may=20 have some motive for this, other than our best interests which = they no=20 doubt are very concerned about?).

This chapter is about=20 =91fuel-less=92 motors. Strictly speaking, they are not = =91self-powered=92=20 but as they don=92t burn a fuel of any kind, in everyday language = they can=20 be described as =91self-powered=92. In the same way that a = solar panel=20 in sunlight uses no fuel and yet puts out electrical power, these = motors=20 draw energy from the environment and provide us with mechanical = power.=20 In actual fact, power is never =93used up=94 but just = converted from=20 one form into another. In the case of our trusty solar = panel, some=20 17% of the radiation from the sun (mainly ultraviolet) is = converted into=20 electrical power and 83% goes in heating and other losses, but as = we don=92t=20 have to supply the sunlight, and the solar panel pours out the = electricity=20 which we want without us having to do anything to make it happen, = we=20 really don=92t care very much about its extremely low efficiency. = As=20 far as we are concerned, the electricity flowing from the panel is = =93free-energy=94.

It is really amazing that we have been = persuaded=20 that we must burn a fuel in order to get power. Take the = case of a=20 heavy-displacement sailing yacht. The skipper can voyage = using his=20 inboard diesel engine:

This = matches perfectly with the thinking that you need to burn a fuel = in order=20 to get power as the yacht is moving along, pushed by the engine = which is=20 powered by burning diesel fuel. But, what if the skipper = decides to=20 switch the engine off and set the sails?:

Now, = the=20 same boat, weighing exactly the same with the same crew, is now = continuing=20 the voyage at the same speed, but no fuel is being burnt. = The=20 really interesting thing is that while we know this perfectly = well, and we=20 are aware that people have sailed right around the world in boats = which do=20 not have engines, it does not seem to occur to us that this shows=20 conclusively that it is not necessary to burn a fuel to power some = item of=20 equipment or form of transport.

In the case of our yacht, = the=20 energy comes from the sun which heats the atmosphere unevenly, = causing=20 winds to blow and the yachtsman uses the sails to make those winds = power=20 his boat through the water. So, a sailing boat is actually = powered=20 by the sun although we don=92t usually think about it that way.=20

There are many hydro-electric =93power stations=94 where = electricity=20 is =91generated=92 by machines driven by water pressure. In = actual=20 fact, no power is =91generated=92 at all, but instead, the = potential energy of=20 the body of water is converted into electricity by having = the water=20 fall and spin the shaft of a machine. So, how did the water = get up=20 there in the first place? Well, it came from rain. = And how=20 did the rain get up there? It rose up there due to = evaporation=20 caused by the heat of the sun. So, the bottom line again is = that=20 hydro-electric =91power=92 stations are powered by the sun. =

Windmills=20 are also powered by the sun. But, and here is the really=20 interesting thing, if I state that it is perfectly possible for a=20 compressed-air engine to produce mechanical power with burning any = fuel,=20 then there is an immediate and strong reaction where people will = say=20 =93Impossible =96 that is perpetual motion !!=94 They imply = that=20 perpetual motion is impossible but never supply any rational = evidence to=20 support that implication. The Earth has been spinning on = its axis=20 for millions of years, so when exactly do they expect it to stop? = =20 All the planets in the Solar System have been orbiting for = millions of=20 years, how long do they have to orbit before they can be = considered to be=20 in perpetual motion? Why then are people so opposed to the = idea of=20 perpetual motion? Presumably, because perpetual motion = shows=20 clearly that a fuel does not have to be burned to =91produce=92 = power and that=20 would not be good for people who sell fuels, and so, we are all = told from=20 an early age that perpetual motion is =93impossible=94. =

Well, that=20 does not matter here as we are going to look at compressed-air = engines=20 which run off the heat of the sun. That is, they are = heat-pumps=20 which are a well accepted engineering fact and they work on wholly = accepted standard scientific principles. An ordinary = refrigerator=20 outputs three or four times as much heat power as the electrical = power=20 driving it, and it could be twice that efficient if it were used = properly.=20 This is a Coefficient Of Performance (COP) of 3 or 4, which = is=20 supposed to be =93impossible=94 but unfortunately, all = refrigerators work like=20 this and you can=92t exactly say that refrigerators don=92t exist, = just=20 because their performance does not appear to fit in with some = theories.=20

Actually, there is no magic involved here as the extra = energy is=20 being drawn from the heat content of the air in the immediate = locality.=20 The refrigerator is not operating in isolation and there is = a heat=20 exchange with the air surrounding it. This outside energy = causes=20 the COP>1 performance. In passing, all COP>1 devices = operate=20 by drawing energy in from an external source (usually the = zero-point=20 energy field) and none of them actually break the =91rules=92 of = science.=20 But, enough of that.

The people who don=92t want = self-powered=20 engines used in the world today, pin their hopes on a continued = ignorance=20 of Engineering facts relating to heat pumps. A = self-sustaining=20 compressed-air engine is actually running off power from the sun = just as=20 sailboats, windmills and hydro-electric power stations do. = Sorry=20 folks, no magic here, just bog-standard Engineering. = Admittedly,=20 very few people know or realise the implications of this standard=20 Engineering:

All work done in compressing air into a storage tank is = converted=20 into heat and then lost to the atmosphere, so the energy in the=20 compressed air inside the tank is the same as that produced by=20 atmospheric heating of that air, but as more of it is now in the = tank,=20 there is additional potential for work to be done. This = extra=20 energy was fed into the air by atmospheric heating before the = air was=20 compressed.

The First Law of Thermodynamics states that = where=20 heat is converted into mechanical energy, or mechanical energy = is=20 converted into heat, the quantity of heat is exactly equivalent = to the=20 amount of mechanical energy. We then have the intriguing=20 situation where all of the mechanical energy put into = compressing air=20 into a storage tank is lost as heat, and yet, the tank contents = now has=20 a higher potential for doing work. This information comes = from=20 Engineering textbooks.
If the expanded cold air leaving the engine is used to cool = the=20 intake air of the compressor, then there will be an added gain = when it=20 warms up inside the cylinder, pulling heat in from the local=20 environment.
If the heat of compression is transferred to the air = container=20 feeding the engine and not given time to dissipate, then there = is a=20 further power gain for the engine.
If compressed air is allowed to expand rapidly, there is a = marked=20 drop in temperature. The Leroy Rogers engine design, = shown later=20 in this chapter, uses this fact to create air-conditioning for a = car=20 driven by a compressed-air engine.

OK then, in broad = outline,=20 the energy available from a tank of compressed air comes directly = from the=20 heat contained in the atmosphere, in spite of the fact that we = always=20 imagine that the energy in the tank was put there by our energetic = pumping.

Let=92s check this out by taking a look at some = of the=20 engines which use these principle to provide fuel-less operation, = starting=20 with the design of Bob Neal specified in his (slightly re-worded) = patent:=20


US Patent 2,030,759		       	      11th Feb. 1936			      Inventor:  Bob =
Neal

COMPRESSOR=20 UNIT

This invention relates to the=20 construction of a compressor, and more particularly to a combined=20 fluid-operated engine and compressor.

The primary object = of the=20 invention, is the provision of a compressor of this character, = wherein=20 there is arranged an automatically counterbalanced crankshaft and = fluid=20 equalisers within a storage tank, which makes it possible for the = engine=20 to operate on constant reserve tank pressure, so as to actuate = additional=20 equipment, the pistons for the engine also being automatically = balanced=20 and suspended when the engine is operating.

Another object = of the=20 invention is the provision of an engine which is operated by air = under=20 pressure, the air being supplied by compressors which are in a = bank with=20 the engine construction.

A further object of this = invention is the=20 provision of an engine of this type of novel construction as the = engine=20 and the compressors are operated from the same crankshaft, which = is of the=20 automatically balanced type, so that high efficiency is attained.=20

A still further object of the invention is the provision = of an=20 engine of this character which is comparatively simple in = construction,=20 thoroughly reliable and efficient in its operation, strong, = durable, and=20 inexpensive to manufacture.

With these and other objects = in view,=20 the invention consists in the features of construction, = combination and=20 arrangement of parts as will be described more fully here, = illustrated in=20 the accompanying drawings which disclose the preferred embodiment = of the=20 invention, and pointed out in the appended Claim.

In the=20 drawings, Fig.1 is a perspective view of the engine = constructed in=20 accordance with the invention.

Fig.2= =20 is a vertical transverse cross-section view through the compressor = part of=20 the engine.

Fig.3= =20 is a vertical cross-sectional view through the power part of the=20 engine.

Fig.4= =20 is a detail elevation of the crankshaft of the engine.

Fig.5= =20 is an enlarged cross-sectional view through one of the electric = heaters=20 for the engine.

Fig.6= =20 is a vertical, longitudinal, cross-sectional view through the air = storage=20 tank, including the equaliser.

The same reference = numbers are=20 used for each individual part in every view in every drawing. =

Referrin= g=20 to the drawings in detail, the engine in its entirety, composes a = cylinder=20 block 10 having inside it, the series of compressor = cylinders=20 11 and the power cylinders 12. The block = 10 is=20 of the V-type and the upper ends of the cylinders are closed off = by the=20 removable heads 13 and 14 which are held in place by = conventional head bolts 15. Beneath block 10 = is the=20 crank case 16, which has detachable plates 17 at = opposite=20 sides, held in place by fasteners 18, and seated so as to = be leak=20 proof. The block 10 is chambered to provide a water = jacket=20 19 surrounding the cylinders, while at the forward end of = the block=20 are water pumps 20, circulating water through the inlet = pipe=20 21 which leads into the jacket and the water exits from the = jacket=20 through the outlet pipe 22. Beside the pumps = 20, is a=20 fan 23 which is operated from the same belt 24 which = drives=20 the pumps.

Working inside the cylinders 11,are the=20 reciprocating pistons 25, their rods 26 sliding = through=20 packing glands 27 and fixed to crossheads 28 which = slide on=20 their mounting guides 29 which are secured to the walls of = the=20 crank case 16. These crossheads 28 are fitted = with=20 wrist pins 30, forming a pivoting connection with the = connecting=20 rods 31, which are connected to their cranks 33 by = their=20 bearings 32. The cranks 33 form part of a = counter=20 balanced crankshaft 34, which is mounted in supports = 35=20 attached to the crank case 16, the shaft being provided = with the=20 required bearings 36.

The = inner=20 ends of the cylinders 11 are fitted with inner end heads = 37,=20 which are provided with air intake ports 38 fitted with = spring ball=20 inlet checks 39, the air entering through passages = 40 which=20 open outside the block 10. Glands 27 are = mounted in=20 the heads 37.

The heads 13 and 37 are = provided with the compressed air outlets 41 and 42, = which=20 are fitted with spring ball checks 43. The heads = 13=20 are also provided with the central air inlets 44, which are = fitted=20 with spring checks 45. Couplings 46 attach = the air=20 outlets 41 and 42 to their outlet feed pipes = 47 and=20 48. These pipes lead to a main conduit 49 = which is=20 located in the centre channel 50 of the block 10. =

At the = rear=20 end of the block 10, mounted on shaft 36, there is a = conventional flywheel 51.

Working = inside the cylinders 12 are the pistons 52, with = their=20 piston rods 53 sliding through packing glands 54 and = fixed=20 in crossheads 55 which slide along their mounting guides = 56,=20 mounted on the inner walls of the crank case 16. The = crossheads=20 55 have wrist pins 57 which provide a pivoting joint = for the=20 connecting rods 58 which are connected by their bearings = 59=20 to their cranks 60 of the crank shaft 34, the inner = ends of=20 the cylinders 12 being closed by the inner heads 61 = and=20 their associated glands 54.

On the cylinders = 12 are=20 slide valve chests 62 in which are the slide valves = 63,=20 these being operated by throw rods 64 actuated by cams = 65=20 and the valves controlling the admission and exhaust of air into = and out=20 of the cylinders 12, through the ports 66 and = 67, and=20 these valves 63 are provided with ports 68 for the = delivery=20 of air under pressure from the inlet passages 69 common to = a pipe=20 70 coming from a compressed air storage tank 71. =

The=20 bottom of the crank case 16 is fitted with a removable = plate=20 72 which is secured in place by fasteners 73, and = when this=20 plate is removed, it provides access to the crank shaft 34 = and the=20 bearings for the engine, as well as other parts inside the crank = case.=20

Leading = into the cylinders 11 are the passages 74 of a = lubricating=20 system (not shown). The compressed air storage tank = 71 has=20 inside it a double-check discharge nozzle 75, supported by = member=20 76. Leading to this equaliser is an air inlet pipe = 77=20 which connects through its valved section 78 to the = compressed air=20 reservoir 79. In the equaliser 75, are the = spaced=20 spring ball checks 80 and 81, one being for the = inlet side=20 and the other for the outlet side of the equaliser. This = pipe=20 77 is connected with the main conduit 49, while a = pipe=20 82 connects to pipe 70. The tank is also = fitted with=20 an automatic relief valve 83 and this valve can be of any = approved=20 type.

Placed=20 around the pipes 70 which connect to the air passages = 69=20 (Fig.3) are electric heating units 84 to heat the=20 pressurised air to above freezing temperature when delivered from = tank=20 71 to the cylinders 12. Supported on the = block=20 10 is an electric generator 85 which is driven from = the=20 shaft 34 (Fig.2) through a belt 24 = (Fig.1) and=20 this generator is included in an electric circuit which also has = the=20 heaters 84 so that these will operate from current supplied = by the=20 generator.

The compressed air storage tank 71 with = the=20 equaliser is constructed so that it is possible to pump air into = it while=20 it contains an air pressure of 200 pounds per square inch while = the=20 compressors are only pumping against 15 pounds per square inch of=20 (atmospheric) pressure. An outside air pressure source can = be=20 coupled with the tank to augment that pressure derived from the = cylinders=20 11 of the engine.

CLAIMS

What = is=20 claimed is:
In a structure of the kind described, a V-shaped = cylinder=20 block provided with upwardly divergent cylinders, end heads fitted = to said=20 cylinders at opposite ends thereof, each head having valved inlets = and=20 outlets, a main outlet lead between the cylinders of the block for = a=20 storage tank and having lateral branches to the outlets at the = inner sides=20 of said heads, one inlet being located at the centre of each head = at the=20 outer ends of said cylinders while the remaining inlets are at the = outer=20 sides of the heads at the inner ends of said cylinders, a = substantially=20 V-shaped crank case fitted to the block beneath the cylinders, a=20 counterbalanced crank shaft journaled in the crank case, pistons = operating=20 in the cylinders and having rods extended into the crank case, = crosshead=20 guides fitted to the interior sides of said case, crossheads = connecting=20 the rods with the guides and sliding on them and connecting rods = operated=20 by the crank shaft and pivoted at the crossheads in order to allow = reciprocation of the pistons.

************************

You will = notice=20 that Bob has avoided any direct mention of the fact that his = engine design=20 is fuel-less. That sort of statement is not popular with = Patent=20 Examiners even if it is perfectly true.

This system could = do with=20 some further explanation, so here is an idea from Scott = Robertson's web site, for a = possible=20 working compressor system using a leaf-blower:

Whil= e=20 this looks rather complicated, in reality it really isn=92t. = Let=92s=20 take the different sections in order:

Firs= t,=20 you have an ordinary air engine, supplied with compressed air from = a=20 pressure tank. This engine exhausts its (cold, expanded) = air to the=20 atmosphere. The engine powers two compressors which between = them=20 keep the tank full of compressed air.

The = first compressor is a simple =91leaf-blower=92 type which produces = a large=20 volume of low-pressure air. The big question is =93how do = you get=20 this large volume of low-pressure air into a tank which has = high-pressure=20 compressed air inside it?=94. Well this seemingly = impossible task is=20 performed by the second compressor aided by a cunning, = ultra-simple=20 design:

Here= ,=20 low-pressure air is fed into the low-pressure area marked in pink. = =20 Separating it from the high-pressure area is a metal plug marked = in green.=20 Set into this plug is a ring of five one-way air valves = marked in=20 red. These one-way valves let the low-pressure air into the = high-pressure area because of a high-speed jet of air produced by = the=20 =91jet-drive compressor=92. At first glance, this seems = impossible, but=20 it is actually just an application of a standard Engineering = technique.=20 The high-speed air jet is directed through a specially = shaped=20 nozzle, creating a local low-pressure zone around the jet: =

The=20 low-pressure air at point =93A=94 flows through the ring of = five=20 one-way valves into the disc-shaped low pressure area = =93B=94 and is=20 blasted into the high-pressure area =93C=94 by the = high-power air jet=20 ripping through the doughnut-shaped ring marked in yellow. = The=20 high-speed air jet causes the low pressure ring =93B=94 by = its rapid=20 movement which creates a vortex due to the shape and positioning = of the=20 doughnut-shaped ring marked in yellow. This clever = arrangement=20 allows large volumes of low-pressure air to be drawn into a tank = which=20 contains high-pressure air.

You will also note that the = two-stage=20 compressor which generates this high-speed jet of air, has its = working=20 area actually inside the tank. This means that the heat of=20 compression is used to heat the air inside the tank and raise its=20 pressure, enhancing the operation further. It should be = borne in=20 mind that the new air entering the system has been heated by the = sun and=20 contains the energy which powers the system. =

The Leroy Rogers Engine.
This=20 engine is driven by compressed air. This principle is very = easily=20 understood and is not a long way from the operation of = steam-powered=20 railway engines of years gone by. What is not generally = realised is=20 that more energy is available from compressed air than the energy = required=20 to compress the air in the first place. Another detail not=20 generally realised is that simple heat energy can be drawn from = the local=20 environment and used to help power the air compressor in a design = of this=20 type.

The Rogers motor shown here makes no claims to = spectacular=20 operation, but in spite of that, Leroy did admit in an interview = that this=20 motor does indeed have a greater output than the applied input, = provided=20 that the motor is not left just ticking over. This motor is = like=20 the US patent 3,744,252 =93Closed Motive Power System Utilising = Compressed=20 Fluids=94 by Eber Van Valkinburg shown below. However, the = Rogers=20 patent shown here has the distinct advantage that it uses = off-the-shelf=20 motors and readily available hardware and there is nothing really = exotic=20 or difficult about the Rogers engine that a person couldn=92t get = from a=20 valve supplier or get a metal fabrication company to construct.=20

Present day vehicle engines are under-geared and run at = fairly low=20 revs. These same engines operate much more efficiently at = higher=20 revs, if they are given different gearing. With the Rogers = motor,=20 the air contained in the high-pressure tank is sufficient to drive = the=20 pistons up and down. The exhaust air can be captured in a = buffer=20 tank and pumped back into the high-pressure tank by a compressor = with much=20 higher gearing and much lower capacity per piston stroke. = The=20 expanded air exiting from the engine is at much lower temperature = than the=20 surrounding air. This gives it higher density and so the=20 re-compression efficiency is raised and in addition, once back in = the=20 storage tank it=92s temperature rises again which boosts the = pressure in the=20 storage tank, courtesy of the heat from the local environment.=20

Here is a slightly re-worded copy of the Lee Rogers = patent:=20

Patent  US 4,292,804 		       6th October 1980  		 =
      Inventor: Leroy K. Rogers

METHOD=20 AND APPARATUS FOR OPERATING AN ENGINE ON COMPRESSED GAS=20

ABSTRACT
The present invention = relates to a=20 method and apparatus for operating an engine having a cylinder = containing=20 a reciprocating piston driven by a compressed gas. The = apparatus=20 comprises a source of compressed gas connected to a distributor = which=20 conveys the compressed gas to the cylinder. A valve is = provided to=20 admit compressed gas to the cylinder when the piston is in an=20 approximately Top Dead Centre position.

In one embodiment = of the=20 present invention, the timing of the opening of the valve is = advanced so=20 that the compressed gas is admitted to the cylinder progressively = further=20 before the Top Dead Centre position of the piston as the speed of = the=20 engine increases.

In a further embodiment of the present=20 invention, a valve actuator is provided which increases the length = of time=20 over which the valve remains open to admit compressed gas to the = cylinder=20 as the speed of the engine increases.

A still further = embodiment=20 of the present invention relates to an apparatus for adapting a=20 conventional internal combustion engine for operation on = compressed gas.=20

US Patent References:

3,881,399	May., 1975	=
Sagi et al.            91/187.
3,885,387	May., 1975	Simington            60/407.
4,018,050	Apr., 1977	 Murphy	                60/412.

DESCRIPTION

BACKGROUND AND SUMMARY OF THE = PRESENT INVENTION

The present invention is a = method and=20 apparatus for operating an engine using a compressed gas as the = motive=20 fluid. More particularly, the present invention relates to = a=20 apparatus for adapting a pre-existing internal combustion engine = for=20 operation on a compressed gas.

Air pollution is one of the = most=20 serious problems facing the world today. One of the major=20 contributors to air pollution is the ordinary internal combustion = engine=20 which is used in most motor vehicles today. Various = devices,=20 including many items required by legislation, have been proposed = in an=20 attempt to limit the pollutants which an internal combustion = engine=20 exhausts to the air. However, most of these devices have = met with=20 limited success and are often both prohibitively expensive and = complex.=20 A clean alternative to the internal combustion engine is = needed to=20 power vehicles and other machinery.

A compressed gas, = preferably=20 air, would provide an ideal motive fluid for an engine, since it = would=20 eliminate the usual pollutants exhausted from an internal = combustion=20 engine. An apparatus for converting an internal combustion = engine=20 for operation on compressed air is disclosed in U.S. Pat. No. = 3,885,387=20 issued May 27, 1975 to Simington. The Simington patent = discloses an=20 apparatus including a source of compressed air and a rotating = valve=20 actuator which opens and closes a plurality of mechanical poppet = valves.=20 The valves deliver compressed air in timed sequence to the=20 cylinders of an engine through adapters located in the spark plug = holes.=20 However, the output speed of an engine of this type is = limited by=20 the speed of the mechanical valves and the fact that the length of = time=20 over which each of the valves remains open cannot be varied as the = speed=20 of the engine increases.

Another apparatus for converting = an=20 internal combustion engine for operation on steam or compressed = air is=20 disclosed in U.S. Pat. No. 4,102,130 issued July 25, 1978 to = Stricklin.=20 The Stricklin patent discloses a device which changes the = valve=20 timing of a conventional four stroke engine such that the intake = and=20 exhaust valves open once for every revolution of the engine = instead of=20 once every other revolution of the engine. A reversing = valve is=20 provided which delivers live steam or compressed air to the intake = valves=20 and is subsequently reversed to allow the exhaust valves to = deliver the=20 expanded steam or air to the atmosphere. A reversing valve = of this=20 type however does not provide a reliable apparatus for varying the = amount=20 of motive fluid injected into the cylinders when it is desired to = increase=20 the speed of the engine. Further, a device of the type = disclosed in=20 the Stricklin patent requires the use of multiple reversing valves = if the=20 cylinders in a multi-cylinder engine were to be fired = sequentially.=20

Therefore, it is an object of the present invention to = provide a=20 reliable method and apparatus for operating an engine or = converting an=20 engine for operation with a compressed gas.

A further = object of=20 the present invention is to provide a method and apparatus which = is=20 effective to deliver a constantly increasing amount of compressed = gas to=20 an engine as the speed of the engine increases.

A still = further=20 object of the present invention is to provide a method and = apparatus which=20 will operate an engine using compressed gas at a speed sufficient = to drive=20 a conventional automobile at highway speeds.

It is still a = further=20 object of the present invention to provide a method and apparatus = which is=20 readily adaptable to a standard internal combustion engine, to = convert the=20 internal combustion engine for operation with a compressed gas.=20

Another object of the invention is to provide a method and = apparatus which utilises cool expanded gas, exhausted from a = compressed=20 gas engine, to operate an air-conditioning unit and/or an = oil-cooler.=20

These and other objects are realised by the method and = apparatus=20 of the present invention for operating an engine having at least = one=20 cylinder containing a reciprocating piston and using compressed = gas as the=20 motive fluid. The apparatus includes a source of compressed = gas, a=20 distributor connected it for conveying the compressed gas to the = cylinder=20 or cylinders. A valve is provided for admitting the = compressed gas=20 to the cylinder when the piston is in an approximately Top Dead = Centre=20 position within the cylinder. An exhaust is provided for = exhausting=20 the expanded gas from the cylinder as the piston returns to = approximately=20 the Top Dead Centre position.

In a preferred embodiment of = the=20 present invention, a device is provided for varying the duration = of each=20 engine cycle over which the valve remains open to admit compressed = gas to=20 the cylinder, dependent upon the speed of the engine. In a = further=20 preferred embodiment of the present invention, an apparatus for = advancing=20 the timing of the opening of the valve is arranged to admit the = compressed=20 gas to the cylinder progressively further and further before the = Top Dead=20 Centre position of the piston, as the speed of the engine = increases.=20

Further features of the present invention include a valve = for=20 controlling the amount of compressed gas admitted to the = distributor.=20 Also, a portion of the gas which has been expanded in the = cylinder=20 and exhausted through the exhaust valve, is delivered to a = compressor to=20 be compressed again and returned to the source of compressed gas. = A=20 gear train can be engaged to drive the compressor selectively at = different=20 operating speeds, depending upon the pressure maintained at the = source of=20 compressed air and/or the speed of the engine. Still = further, a=20 second portion of the exhaust gas is used to cool a lubricating = fluid for=20 the engine or to operate an air-conditioning unit.

In a = preferred=20 embodiment of the present invention, the valve for admitting = compressed=20 gas to the cylinder is operated electrically. The device = for=20 varying the duration of each engine cycle, over which the intake = valve=20 remains open, as the speed of the engine increases, comprises a = rotating=20 element whose effective length increases as the speed of the = engine=20 increases, causing a first contact on the rotating element to be=20 electrically connected to a second contact on the rotating = element, for a=20 longer period of each engine cycle. The second contact = operates the=20 valve causing it to remain in an open position for a longer period = of each=20 engine cycle, as the speed of the engine increases.

Still = further=20 features of the present invention include an adaptor plate for = supporting=20 the distributor above the intake manifold of a conventional = internal=20 combustion engine after a carburettor has been removed to allow = air to=20 enter the cylinders of the engine through the intake manifold and=20 conventional intake valves. Another adaptor plate is = arranged over=20 an exhaust passageway of the internal combustion engine to reduce = the=20 cross-sectional area of the exhaust passageway. =

BRIEF=20 DESCRIPTION OF THE DRAWINGS
Preferred embodiments of a = method=20 and apparatus for operating an engine according to the present = invention=20 will be described with reference to the accompanying drawings in = which=20 components have the same reference numbers in each drawing.=20

Fig.1 is a schematic representation of an apparatus = according to the present invention arranged on an engine:

<= B>Fig.2=20 is a side view of one embodiment of a valve actuator according to = the=20 present invention.

Fi= g.3=20 is a cross-sectional view taken along the line 3--3 in=20 Fig.2.

<= B>Fig.4=20 is a cross-sectional view of a second embodiment of a valve = actuator=20 according to the present invention.

<= B>Fig.5=20 is a view taken along the line 5--5 in Fig.4.

<= B>Fig.6=20 is a cross-sectional view of a third embodiment of a valve = actuator=20 according to the present invention;

<= B>Fig.7=20 is a view taken along the line 7--7 in Fig.6.

<= B>Fig.8=20 is a cross-sectional view of a gearing unit to drive a compressor=20 according to the present invention.

<= BR>DETAILED=20 DESCRIPTION OF THE PREFERRED EMBODIMENTS

With = reference to=20 Fig.1, an engine block 21 (shown in phantom) having = two=20 banks of cylinders with each bank including cylinders 20 = having=20 pistons 22 which reciprocate in them in a conventional = manner (only=20 one of which is shown in phantom). While the illustrated = engine is=20 a V-8 engine, it will be apparent that the present invention is = applicable=20 to an engine having any number of pistons and cylinders with the = V-8=20 engine being utilised for illustration purposes only. A = compressed=20 gas tank 23 is provided to store a compressed gas at high = pressure.=20 It may also be desirable to include a small electric or gas = compressor to provide compressed gas to supplement the compressed = gas held=20 in the tank 23. In a preferred embodiment, the = compressed=20 gas is air which can be obtained from any suitable source. =

A= =20 line 25 transports the gas withdrawn from the tank = 23 when a=20 conventional shut-off valve 27 is open. In addition, = a=20 solenoid valve 29 preferably operated by a suitable = key-operated=20 engine switch (not shown) is also placed in the line 25. = In=20 normal operation, the valve 27 is maintained open at all = times with=20 the solenoid valve 29 operating as a selective shut off = valve to=20 start and stop the engine 21.

A suitable regulating = valve=20 31 is arranged downstream of the solenoid valve 29 = and is=20 connected by a linkage 33 to a throttle linkage 35 = which is=20 operator-actuated by any suitable apparatus such as a foot pedal = (not=20 shown). The line 25 enters an end of a distributor = 33=20 and is connected to an end of a pipe 35 which is closed at = the=20 other end. A plurality of holes, which are equal to the = number of=20 cylinders in the engine 21, are provided on either side of = the pipe=20 35 along the length of the pipe 35.

When the = present=20 invention is used to adapt a conventional internal combustion = engine for=20 operation on compressed gas, an adaptor plate 36 is = provided to=20 support the distributor 33 in spaced relation from the = usual intake=20 opening in the intake manifold of the engine after a conventional=20 carburettor has been removed. In this way, air is permitted = to=20 enter the internal combustion engine through the usual passageways = and to=20 be admitted to the cylinders through suitable intake valves (not = shown).=20 The adaptor plate 36 is attached to the engine block = 21 and the distributor 33 by any suitable apparatus, = e.g.,=20 bolts.

Each of the holes in the pipe 35 is = connected in=20 fluid-tight manner to a single line 37. Each line = 37=20 carries the compressed gas to a single cylinder 20. = In a=20 preferred embodiment, each of the lines 37 is 1/2 inch high = pressure plastic tubing attached through suitable connectors to = the=20 distributor 33 and the pipe 35. Each of the = lines=20 37 is connected to a valve 39 which is secured in an = opening=20 provided near the top of each of the cylinders 20. = In the=20 case of a conversion of a standard internal combustion engine, the = valves=20 39 can be conveniently screwed into a tapped hole in the = cylinder=20 20 typically provided for a spark plug of the internal = combustion=20 engine. In a preferred embodiment, the valves 39 are = solenoid actuated valves in order to provide a fast and reliable = opening=20 and closing of the valves 39.

Each of the valves = 39=20 is energised by a valve actuator 41 through one of a = plurality of=20 wires 43. The valve actuator 41 is driven by = a shaft=20 of the engine similar to the drive for a conventional distributor = of an=20 internal combustion engine. That is, a shaft 55 of = the valve=20 actuator 41 is driven in synchronism with the engine = 21 at=20 one half the speed of the engine 21.

A = first=20 embodiment of the valve actuator 41 (Fig.2 and=20 Fig.3), receives electrical power through a wire 45 = which is=20 energised in a suitable manner by a battery, and a coil if = necessary (not=20 shown) as is conventional in an internal combustion engine. = The=20 wire 45 is attached to a central post 47 by a nut = 49.=20 The post 47 is connected to a conducting plate = 51=20 arranged in a housing 53 for the valve actuator 41. = =20 Within the housing 53, the shaft 55 has an = insulating=20 element 57 secured to an end of the shaft 55 and = rotates=20 with it when the shaft 55 is driven by the engine = 21. =20 A first end of a flexible contact 59 is continuously biased = against=20 the conducting plate 51 to receive electricity from the = battery or=20 other suitable source. The other end of the contact = 59 is=20 connected to a conducting sleeve 60 which is in constant = contact=20 with a spring biased contact 61 which is arranged within = the sleeve=20 60. The contact 61 is pressed by a spring = 63=20 which pushes contact 61 towards a side wall of the housing=20 53.

With = reference to Fig.3, a plurality of contacts 65 are = spaced=20 from one another and are arranged around the periphery of the = housing=20 53 at the same level as the spring biased contact = 61. =20 Each contact 65 is electrically connected to a post = 67 which=20 extends outside of the housing 53. The number of = contacts=20 65 is equal to the number of cylinders in the engine = 21.=20 One of the wires 43, which actuate the valves = 39, is=20 secured to each of the posts 67.

In operation, as = the shaft=20 55 rotates in synchronism with the engine 21, the = insulating=20 element 57 rotates and electricity is ultimately delivered = to=20 successive pairs of the contacts 65 and wires 43 = through the=20 spring loaded contact 61 and the flexible contact = 59. =20 In this way, each of the electrical valves 39 is activated = and=20 opened in the proper timed sequence to admit compressed gas to = each of the=20 cylinders 20 to drive the pistons 22 on a downward = stroke.=20

The embodiment illustrated in Fig.2 and = Fig.3 is=20 effective in causing each of the valves 39 to remain open = for a=20 long enough period of time to admit sufficient compressed gas to = each of=20 the cylinders 20 of the engine 21 to drive the = engine=20 21. The length of each of the contacts 65 = around the=20 periphery of the housing 53 is sufficient to permit the = speed of=20 the engine to be increased when desired by the operator by moving = the=20 throttle linkage 35 which actuates the linkage 33 to = further=20 open the regulating valve 31 to admit more compressed gas = from the=20 tank 23 to the distributor 33. However, it = has been=20 found that the amount of air admitted by the valves 39 when = using=20 the first embodiment of the valve actuator 41 (Fig.2 = and=20 Fig.3) is substantially more than required to operate the = engine=20 21 at an idling speed. Therefore, it may be = desirable to=20 provide a valve actuator 41 which is capable of varying the = duration of each engine cycle over which the solenoid valves = 39 are=20 actuated, i.e., remain open to admit compressed gas, as the speed = of the=20 engine 21 is varied.

A = second=20 embodiment of a valve actuator 41 which is capable of = varying the=20 duration of each engine cycle over which each of the valves = 39=20 remains open to admit compressed gas to the cylinders 20 = dependent=20 upon the speed of the engine 21 will be described with = reference to=20 Fig.4 and Fig.5 wherein members corresponding to = those of=20 Fig.2 and Fig.3 bear like reference numbers. = The wire=20 45 from the electricity source is attached to the post = 47 by=20 the nut 49. The post 47 has a annular contact = ring=20 69 electrically connected to an end of the post 47 = and=20 arranged within the housing 53. The shaft 55 = rotates=20 at one half the speed of the engine as in the embodiment of = Fig.2=20 and Fig.3.

At = an=20 upper end of the shaft 55, a splined section 71 = receives a=20 sliding insulating member 73. The splined section = 71=20 of the shaft 55 holds the insulating member 73 = securely as=20 it rotates with shaft 55 but permits the insulating member=20 73 to slide axially along the length of the splined section = 71. Near the shaft 55, a conductive sleeve = 72=20 is arranged in a bore 81 in an upper surface of the = insulating=20 element 73 generally parallel to the splined section = 71.=20 A contact 75, biased towards the annular contact = ring=20 69 by a spring 77, is arranged within the conductive = sleeve=20 72 and in contact with it. The conductive sleeve = 72=20 also contacts a conductor 79 at a base of the bore = 81.=20

The conductor 79 extends to the upper surface of = the=20 insulating element 73 near an outer periphery of the = insulating=20 element 73 where the conductor 79 is electrically = connected=20 to a flexible contact 83. The flexible contact = 83=20 connects, one after the other, with a series of radial contacts = 85=20 which are positioned on an upper inside surface of the housing = 53.=20 A weak spring 87 arranged around the splined section = 71 engages a stop member 89 secured on the shaft = 55=20 and the insulating element 73 to slightly bias the = insulating=20 element 73 towards the upper inside surface of the housing=20 53 to ensure contact between the flexible contact 83 = and the=20 upper inside surface of the housing 53. As best seen = in=20 Fig.5, the radial contacts 85 on the upper inside = surface of=20 the housing 53 are arranged generally in the form of radial = spokes=20 extending from the centre of the housing 53 with the number = of=20 contacts being equal to the number of cylinders 20 in the = engine=20 21. The number of degrees covered by each of the = radial=20 contacts 85 gradually increases as the distance from the = centre of=20 the upper inside surface of the housing 53 increases. =

In=20 operation of the device of Fig.4 and Fig.5, as the = shaft=20 55 rotates, electricity flows along a path through the wire = 45 down through post 47 to the annular contact = member=20 69 which is in constant contact with the spring biased = contact=20 75. The electrical current passes through the = conductive=20 sleeve 72 to the conductor 79 and then to the = flexible=20 contact 83. As the flexible contact 83 = rotates along=20 with the insulating member 73 and the shaft 55, the = tip of=20 the flexible contact 83 successively engages each of the = radial=20 contacts 85 on the upper inside of the housing 53. = As=20 the speed of the shaft 55 increases, the insulating member=20 73 and the flexible contact 83 attached to it, move = upwards=20 along the splined section 71 of the shaft 55 due to = the=20 radial component of the splines in the direction of rotation under = the=20 influence of centrifugal force. As the insulating member = 73=20 moves upwards, the flexible contact 83 is bent so that the = tip of=20 the contact 83 extends further outwards radially from the = centre of=20 the housing 53 (as seen in phantom lines in Fig.4). = =20 In other words, the effective length of the flexible contact = 83=20 increases as the speed of the engine 21 increases. =

As the=20 flexible contact 83 is bent and the tip of the contact = 83=20 moves outwards, the tip remains in contact with each of the radial = contacts 85 for a longer period of each engine cycle due to = the=20 increased angular width of the radial contacts with increasing = distance=20 from the centre of the housing 53. In this way, the = length=20 of time over which each of the valves 39 remains open is = increased=20 as the speed of the engine is increased. Thus, a larger = quantity of=20 compressed gas or air is injected into the cylinders as the speed=20 increases. Conversely, as the speed decreases and the = insulating=20 member 73 moves downwards along the splined section = 71, a=20 minimum quantity of air is injected into the cylinder due to the = shorter=20 length of the individual radial contact 85 which is in = contact with=20 the flexible contact 83. In this way, the amount of=20 compressed gas that is used during idling of the engine 21 = is at a=20 minimum whereas the amount of compressed gas which is required to = increase=20 the speed of the engine 21 to a level suitable to drive a = vehicle=20 on a highway is readily available.

Shown= in=20 Fig.6 and Fig.7, is a third embodiment of a valve = actuator=20 41 according to the present invention. This = embodiment=20 includes a curved insulating element 91 having it=92s first = end able=20 to pivot, being secured by any suitable device such as screw = 92 to=20 the shaft 55 for co-rotation with the shaft 55. = The=20 screw 92 is screwed into a tapped hole in the insulating = element=20 91 so that a tab 94 at an end of the screw 92 = engages=20 a groove 96 provided in the shaft 55. In this = way,=20 the insulating element 91 rotates positively with the shaft = 55. However, as the shaft 55 rotates faster, = the=20 other end 98 of the insulating element 91 is = permitted to=20 pivot outwards under the influence of centrifugal force because of = the=20 groove 96 provided in the shaft 55. A spring=20 93, connected between the second end 98 of the = element=20 91 and the shaft 55 urges the second end of the = element=20 91 towards the centre of the housing 53.

A=20 contact 99 similar to the contact 59 (Fig.2) = is=20 arranged so that one end of the contact piece 99 is in = constant=20 contact with the conducting plate 51 located centrally = within the=20 housing 53. The other end of the contact 99 = engages a=20 conductive sleeve 101 arranged in bore 102. A = contact=20 element 95 is arranged in the conductive sleeve 101 = in=20 constant contact with the sleeve 101. The bore = 102 is=20 arranged generally parallel to the shaft 55 near the second = end of=20 the curved insulating element 91. The contact = 95 is=20 biased by a spring 97 towards the upper inside surface of = the=20 housing 53 for selective contact with each of the plurality = of=20 radial contacts 85 which increase in arc length towards the = outer=20 peripheral surface of the housing 53 (Fig.6). =

When=20 the device shown in Fig.6 and Fig.7 is operating, as = the=20 shaft 55 rotates the curved insulating element 91 = rotates=20 with the shaft 55 and the second end 98 of the = insulating=20 element 91 tends to pivot about the shaft 55 due to=20 centrifugal force. Thus, as the effective length of the = contact=20 95 increases, i.e., as the curved insulating element = 91=20 pivots further outwards, the number of degrees of rotation over = which the=20 contact 95 is in contact with each of the radial contacts = 85=20 on the upper inside surface of the housing 53 increases = thereby=20 allowing each of the valves 39 to remain open for a longer = period=20 of each engine cycle, which in turn, allows more compressed gas = enter the=20 respective cylinder 20 to further increase the speed of the = engine=20 21.

With reference to Fig.1, a mechanical = advance=20 linkage 104 which is connected to the throttle linkage = 35,=20 advances the initiation of the opening of each valve 39 = such that=20 compressed gas is injected into the respective cylinder further = before the=20 piston 22 in the respective cylinder 20 reaches a = Top Dead=20 Centre position as the speed of the engine is increased by moving = the=20 throttle linkage 35. The advance linkage 104 = is=20 similar to a conventional standard mechanical advance employed on = an=20 internal combustion engine. In other words, the linkage = 104=20 varies the relationship between the angular positions of a point = on the=20 shaft 55 and a point on the housing 53 containing = the=20 contacts. Alternatively, a conventional vacuum advance = could also=20 be employed. By advancing the timing of the opening of the = valves=20 39, the speed of the engine can more easily be increased.=20

The operation of the engine cycle according to the present = invention will now be described. The compressed gas = injected into=20 each cylinder of the engine 21 drives the respective piston = 22 downwards to rotate a conventional crankshaft (not = shown).=20 The movement of the piston downwards causes the compressed = gas to=20 expand rapidly and cool. As the piston 22 begins to = move=20 upwards in the cylinder 20 a suitable exhaust valve (not = shown),=20 arranged to close an exhaust passageway, is opened by any suitable = apparatus. The expanded gas is then expelled through the = exhaust=20 passageway. As the piston 22 begins to move = downwards again,=20 a suitable intake valve opens to admit ambient air to the = cylinder. =20 The intake valve closes and the ambient air is compressed on the=20 subsequent upward movement of the piston until the piston reaches=20 approximately the Top Dead Centre position at which time the = compressed=20 gas is again injected into the cylinder 20 to drive the = piston=20 22 downwards and the cycle begins again.

In the = case of=20 adapting a conventional internal combustion engine for operation = on=20 compressed gas, a plurality of plates 103 are arranged, = preferably=20 over an end of the exhaust passageways, in order to reduce the = outlet size=20 of the exhaust passageways of the conventional internal combustion = engine.=20 In the illustrated embodiment, a single plate having an = opening in=20 the centre is bolted to the outside exhaust passageway on each = bank of the=20 V-8 engine, while another single plate having two openings in it, = is=20 arranged with one opening over each of the interior exhaust = passageways on=20 each bank of the V-8 engine. A line 105 is suitably = attached=20 to each of the adaptor plates to carry the exhaust to an = appropriate=20 location. In a preferred embodiment, the exhaust lines = 105=20 are made from 1.5" plastic tubing.

In a preferred = embodiment, the=20 exhaust lines 105 of one bank of the V-8 engine are = collected in a=20 line 107 and fed to an inlet of a compressor 109. = The=20 pressure of the exhaust gas emanating from the engine 21 = according=20 to the present invention is approximately 25 p.s.i. In this = way,=20 the compressor 109 does not have to pull the exhaust into = the=20 compressor since the gas exhausted from the engine 21 is at = a=20 positive pressure. The positive pressure of the incoming = fluid=20 increases the efficiency and reduces wear on the compressor = 109.=20 The exhaust gas is compressed in the compressor 109 = and=20 returned through a line 111 and a check valve 113 to = the=20 compressed gas storage tank 23. The check valve = 113=20 prevents the flow of compressed gas stored in the tank 23 = back=20 towards the compressor 109.

A suitable pressure = sensor=20 115 is arranged at an upper end of the tank 23 and = sends a=20 signal along a line 117 when the pressure exceeds a = predetermined=20 level and when the pressure drops below a predetermined level. = The=20 line 117 controls an electrically activated clutch = 119=20 positioned at the front end of the compressor 109. = The=20 clutch 119 is operated to engage and disengage the = compressor=20 109 from a drive pulley 121. Also, the signal = carried=20 by the line 117 activates a suitable valve 123 = arranged on=20 compressor housing 125 to exhaust the air entering the = compressor=20 housing 125 from the line 107 when the clutch = 119 has=20 disengaged the compressor 109 from the drive pulley = 121.=20

In a preferred embodiment, when the pressure is the tank = 23=20 reaches approximately 600 p.s.i., the clutch 119 is = disengaged and=20 the compressor 109 is deactivated and the valve 123 = is=20 opened to exhaust the expanded gas delivered to the compressor = 109=20 from the line 107 to the atmosphere. When the = pressure=20 within the tank 23 drops below approximately 500 p.s.i., = the sensor=20 115 sends a signal to engage the clutch 119 and = close the=20 valve 123, thereby operating the compressor 109 for=20 supplying the tank 23 with compressed gas.

The = pulley=20 121 which drives the compressor 109 through the = clutch=20 119 is driven by a belt 127 which is driven by a = pulley=20 129 which operates through a gear box 131. = With=20 reference to Fig.1 and Fig.8, a second pulley = 133 on=20 the gear box is driven by a belt 135 from a pulley = 137=20 arranged on a drive shaft 139 of the engine 21. The = pulley=20 137 drives a splined shaft 140 which has a first = gear=20 141 and a second larger gear 143 placed on it, which = rotates=20 with the splined shaft 140. The splined shaft = 140=20 permits axial movement of the gears 141 and 143 = along the=20 shaft 140.

In=20 normal operation (as seen in Fig.8), the first gear = 141=20 engages a third gear 145 arranged on a shaft 147 = which=20 drives the pulley 129. The shafts 140 and = 147=20 are arranged in suitable bearings 149 positioned at each = end of it.=20 When the speed of the engine 21 drops below a = predetermined=20 level, a suitable sensor 151 responsive to the speed of the = drive=20 shaft 139 of the engine 21 generates a signal which = is=20 transmitted through a line 153 to a solenoid actuator = 155=20 arranged within the gear box 131. The solenoid = actuator=20 155 moves the first and second gears 141, 143 = axially along=20 the splined shaft 140 to the right as seen in Fig.8 = so that=20 the second, larger gear 143 engages a fourth smaller gear=20 157 which is arranged on the shaft 147. The = ratio of=20 the second gear 143 to the fourth gear 157 is = preferably=20 approximately 3 to 1.

In this way, when the speed of the = engine=20 21 drops below the predetermined level as sensed by the = sensor=20 151 (which predetermined level is insufficient to drive the = compressor 109 at a speed sufficient to generate the = 500-600 pounds=20 of pressure which is preferably in the tank 23), the = solenoid=20 actuator 155 is energised to slide the gears 143, = 141=20 axially along the splined shaft 140 so that the second, = larger gear=20 143 engages the fourth, smaller gear 157 to drive = the pulley=20 129 and hence the compressor 109 at a higher rate, = to=20 generate the desired pressure. When the speed of the engine = increases above the predetermined level, which, in a preferred = embodiment=20 is approximately 1500 rpm, the solenoid actuator 155 is = deactivated=20 by the sensor 151 thereby moving the gears 143 and=20 141 to the left as seen in Fig.8 so that the first = gear=20 141, engages again with the third gear 145 to = effectuate a 1=20 to 1 ratio between the output shaft 139 of the engine = 21 and=20 the pulley 129.

The other bank of the V-8 engine = has its=20 exhaust ports arranged with adapter plates 103 similar to = those on=20 the first bank. However, the exhaust from this bank of the = engine=20 21 is not collected and circulated through the compressor=20 109. In a preferred embodiment, a portion of the = exhaust is=20 collected in a line 159 and fed to an enlarged chamber = 161.=20 A second fluid is fed through a line 163 into the = chamber=20 161 to be cooled by the cool exhaust emanating from the = engine=20 21 in the line 159. The second fluid in the = line=20 163 may be either transmission fluid contained in a = transmission=20 associated with the engine 21 or a portion of the oil used = to=20 lubricate the engine 21. A second portion of the = exhaust=20 from the second bank of the V-8 engine is removed from the line = 159=20 in a line 165 and used as a working fluid in an air = conditioning=20 system or for any other suitable use.

It should be noted = that the=20 particular arrangement utilised for collecting and distributing = the gas=20 exhausted from the engine 21 would be determined by the use = for=20 which the engine is employed. In other words, it may be=20 advantageous to rearrange the exhaust tubing such that a larger or = smaller=20 percentage of the exhaust is routed through the compressor = 109.=20 It should also be noted that since the exhaust lines = 105 are=20 plastic tubing, a rearrangement of the lines for a different = purpose is=20 both simple and inexpensive.

In operation of the engine of = the=20 present invention, the engine 21 is started by energising = the=20 solenoid valve 29 and any suitable starting device (not = shown),=20 e.g., a conventional electric starter as used on an internal = combustion=20 engine. Compressed gas from the full tank 23 flows = through=20 the line 25 and a variable amount of the compressed gas is = admitted=20 to the distributor 33 by controlling the regulator valve = 31=20 through the linkage 33 and the operator actuated throttle = linkage=20 35. The compressed gas is distributed to each of the = lines=20 37 which lead to the individual cylinders 20. = The=20 compressed gas is admitted to each of the cylinders 20 in = timed=20 relationship to the position of the pistons within the cylinders = by=20 opening the valves 39 with the valve actuator 41.=20

When it is desired to increase the speed of the engine, = the=20 operator moves the throttle linkage 35 which simultaneously = admits=20 a larger quantity of compressed gas to the distributor 33 = from the=20 tank 23 by further opening the regulator valve 31. = =20 The timing of the valve actuator 41 is also advanced = through the=20 linkage 104. Still further, as the speed of the = engine=20 21 increases, the effective length of the rotating contact=20 83 (Fig.4) or 95 (Fig.6) increases = thereby=20 electrically contacting a wider portion of one of the stationary = radial=20 contacts 85 to cause each of the valves 39 to remain = open=20 for a longer period of each engine cycle to admit a larger = quantity of=20 compressed gas to each of the cylinders 20.

As can = be seen,=20 the combination of the regulating valve 31, the mechanical = advance=20 104, and the valve actuator 41, combine to produce a = compressed gas engine which is quickly and efficiently adaptable = to=20 various operating speeds. However, all three of the = controls need=20 not be employed simultaneously. For example, the mechanical = advance=20 104 could be utilised without the benefit of one of the = varying=20 valve actuators 41 but the high speed operation of the = engine may=20 not be as efficient. By increasing the duration of each = engine=20 cycle over which each of the valves 39 remains open to = admit=20 compressed gas to each of the cylinders 20 as the speed = increases,=20 conservation of compressed gas during low speed operation and = efficient=20 high speed operation are both possible.

After the = compressed gas=20 admitted to the cylinder 20 has forced the piston 22 = downwards within the cylinder to drive the shaft 139 of the = engine,=20 the piston 22 moves upwards within the cylinder 20 = and=20 forces the expanded gas out through a suitable exhaust valve (not = shown)=20 through the adapter plate 103 (if employed) and into the = exhaust=20 line 105. The cool exhaust can then be collected in = any=20 suitable arrangement to be compressed and returned to the tank = 23=20 or used for any desired purpose including use as a working fluid = in an air=20 conditioning system or as a coolant for oil.

When using = the=20 apparatus and method of the present invention to adapt a ordinary = internal=20 combustion engine for operation with compressed gas it can be seen = that=20 considerable savings in weight are achieved. For example, = the=20 ordinary cooling system including a radiator, fan, hoses, etc. can = be=20 eliminated since the compressed gas is cooled as it expands in the = cylinder. In addition, there are no explosions within the = cylinder=20 to generate heat. Further reductions in weight are obtained = by=20 employing plastic tubing for the lines which carry the compressed = gas=20 between the distributor and the cylinders and for the exhaust = lines.=20 Once again, heavy tubing is not required since there is = little or=20 no heat generated by the engine of the present invention. = In=20 addition, the noise generated by an engine according to the = present=20 invention is considerably less than that generated by an ordinary = internal=20 combustion engine since there are no explosions taking place = within the=20 cylinders.

The principles of preferred embodiments of the = present=20 invention have been described in the foregoing specification. = =20 However, the invention which is intended to be protected is not to = be=20 construed as limited to the particular embodiments disclosed. = The=20 embodiments are to be regarded as illustrative rather than = restrictive.=20 Variations and changes may be made by others without = departing from=20 the spirit of the invention. Accordingly, it is expressly = intended=20 that all such variations and changes which fall within the spirit = and the=20 scope of the present invention as defined in the appended claims = be=20 embraced thereby.

**********************

This patent shows = how the=20 practical details of running an engine on compressed air can be = dealt=20 with. What it does not show is background details of the = actual=20 energy flows and the effects of compressing air and then letting = it=20 expand. These things are not normally encountered in our = daily=20 lives and so we do not have an immediate intuitive feel for how a = system=20 like these will operate. Take the effects of expansion. = =20 While it is quite well known that letting a compressed gas expand = causes=20 cooling, the practical effect is seldom realised.

This web = site show the details of a =93vortex tube=94 which is a = completely passive=20 device with no moving parts:

This= =20 device does things which you would not expect. Compressed = air at a=20 normal temperature of, say, seventy degrees Centigrade is fed into = the=20 circular chamber where the shape of the chamber causes it to = spiral=20 rapidly as it exits the tube:

Ther= e=20 is an energy gain in a vortex, as can be seen in a hurricane or = tornado,=20 but the really interesting thing here is the dramatic change in=20 temperature caused by the change in pressure as the air expands. = =20 The ratio of heat gain to heat loss is controlled by the ratio of = the=20 sizes of the openings, which is why there is an adjustable nozzle = on the=20 small opening.

The air exiting through the large opening = is much=20 higher volume than the air exiting through the small opening and = it=20 expands very rapidly, producing a massive drop in temperature. = The=20 density of this cold air is now much higher than the air entering = the=20 vortex chamber. So there has been both a drop in = temperature and an=20 increase in density. These features of the expansion are = made use=20 of in the Leroy Rogers engine design, where some of the expanded = air=20 exhaust of the engine is compressed and passed back to the main = air=20 storage tank. While the compressor does raise the air = temperature=20 as it pumps the air back into the tank, it does not reach its = original=20 temperature instantly.

This results in the air temperature = inside=20 the tank dropping as the engine operates. But, the lowered = tank=20 temperature causes an inflow of heat from its immediate = environment,=20 raising the overall tank temperature again. This warming of = the=20 chilled air causes the tank pressure to increase further, giving = an energy=20 gain, courtesy of the local environment. It is important to = understand that it takes less energy to compress air than the = kinetic=20 energy which can be generated by letting that compressed air = expand again.=20 This is a practical situation, courtesy of the local = environment=20 and is not a breach of the law of Conservation of Energy. = It is=20 also a feature which has not yet been exploited to any great = degree and=20 which is just waiting to be used by any adventurous inventor or=20 experimenter.

The Eber Van = Valkinburg=20 Engine.
Eber presents a custom engine = based on=20 these principles. His engine uses both compressed air and=20 compressed oil to manipulate pressures within the system and = provide an=20 engine which is self-powered. Here is a slightly re-worded = copy of=20 the Eber Van Valkinburg patent:

Patent  US 3,744,252                            =
10th July 1973                            Inventor: Eber Van =
Valkinburg

CLOSED=20 MOTIVE POWER SYSTEM UTILISING COMPRESSED=20 FLUIDS

ABSTRACT
Stored energy in = a=20 compressed elastic fluid is utilised in a controlled manner to = pressurise=20 an inelastic fluid and to maintain such pressurisation. The = pressurised inelastic fluid is throttled to the impeller of a = prime mover.=20 Only a portion of the output energy from the prime mover is = utilised to circulate the inelastic fluid so as to maintain a = nearly=20 constant volumetric balance in the system.=20

DESCRIPTION
The objective of the = invention is to=20 provide a closed-loop power system which utilises the expansive = energy of=20 a compressed elastic fluid, such as air, to pressurise and = maintain=20 pressurised throughout the operational cycle of the system a = second=20 non-elastic and non-compressible fluid, such as oil. The=20 pressurised non-elastic fluid is released in a controlled manner = by a=20 throttle to the rotary impeller of a turbine or the like, having = an output=20 shaft. This shaft is coupled to a pump for the non-elastic = fluid=20 which automatically maintains the necessary circulation needed for = the=20 operation of the prime mover, and maintains a near volumetric = balance in=20 the system between the two fluids which are separated by = self-adjusting=20 free piston devices. The pump for the non-elastic fluid = includes an=20 automatic by-pass for the non-elastic fluid which eliminates the=20 possibility of starving the pump which depends on the discharge of = the=20 non-elastic fluid at low pressure from the exhaust of the turbine. = =20 Other features and advantages of the invention will become = apparent during=20 the course of the following detailed description. =

BRIEF=20 DESCRIPTION OF DRAWING FIGURES
Fig.1 is a partly = schematic=20 cross-sectional view of a closed motive power system embodying the = invention.

F= ig.2=20 is a fragmentary perspective view of a rotary prime mover utilised = in the=20 system. Fig.3 is an enlarged fragmentary vertical section = through=20 the prime mover taken at right angles to its rotational axis. = Fig.4=20 is an enlarged fragmentary vertical section taken on line = 4--4 of=20 Fig.1. Fig.5 is a similar section taken on line = 5--5=20 of Fig.4.

DETAILED DESCRIPTION

Refe= rring=20 to the drawings in detail, in which the same numbers refer to the = same=20 parts in each drawing, the numeral 10 designates a supply = bottle or=20 tank for a compressed elastic fluid, such as air. = Preferably, the=20 air in the bottle 10 is compressed to approximately 1,500 = p.s.i.=20 The compressed air from the bottle 10 is delivered = through a=20 suitable pressure regulating valve 11 to the chamber = 12 of a=20 high pressure tank 13 on one side of a free piston = 14 in the=20 bore of such tank. The free piston 14 separates the = chamber=20 12 for compressed air from a second chamber 15 for = an=20 inelastic fluid, such as oil, on the opposite side of the free = piston.=20 The free piston 14 can move axially within the bore = of the=20 cylindrical tank 13 and is constantly self-adjusting there = to=20 maintain a proper volumetric balance between the two separated = fluids of=20 the system. The free piston has the ability to maintain the = two=20 fluids, air and oil, completely separated during the operation of = the=20 system.

The regulator valve 11 delivers compressed = air to=20 the chamber 12 under a pressure of approximately 500 p.s.i. = =20 The working inelastic fluid, oil, which fills the chamber = 15 of=20 high pressure tank 13 is maintained under 500 p.s.i. = pressure by=20 the expansive force of the elastic compressed air in the chamber = 12=20 on the free piston 14. The oil in the chamber = 15 is=20 delivered to a prime mover 16, such as an oil turbine, = through a=20 suitable supply regulating or throttle valve 17 which = controls the=20 volume of pressurised oil delivered to the prime mover. =

The=20 turbine 16 embodies a stator consisting of a casing ring = 18=20 and end cover plates 19 joined to it in a fluid- tight = manner.=20 It further embodies a single or plural stage impeller or = rotor=20 having bladed wheels 20, 21 and 22 in the = illustrated=20 embodiment. The peripheral blades 23 of these = turbine wheels=20 receive the motive fluid from the pressurised chamber 15 = through=20 serially connected nozzles 24, 25 and 26, connected=20 generally tangentially through the stator ring 18, as shown = in=20 Fig.3. The first nozzle 24 shown = schematically in=20 Fig.1 is connected directly with the outlet of the throttle = valve=20 17. The successive nozzles 25 and 26 = deliver=20 the pressurised working fluid serially to the blades 23 of = the=20 turbine wheels 21 and 22, all of the turbine wheels = being=20 suitably coupled to a central axial output or working shaft = 27 of=20 the turbine 16.

Back= -pressure=20 sealing blocks 28, made of fibre, are contained within = recesses=20 29 of casing ring 18 to prevent co-mingling of the = working=20 fluid and exhaust at each stage of the turbine. A = back-pressure=20 sealing block 28 is actually only required in the third = stage=20 between inlet 26 and exhaust 31, because of the = pressure=20 distribution, but such a block can be included in each stage as = shown in=20 Fig.1. The top surface, including a sloping face = portion=20 30 on each block 28, reacts with the pressurised = fluid to=20 keep the fibre block sealed against the adjacent, bladed turbine = wheel;=20 and the longer the slope on the block to increase it=92s top = surface area,=20 the greater will be the sealing pressure pushing it against the = periphery=20 of the wheel.

Leading from the final stage of the turbine=20 16 is a low-pressure working fluid exhaust nozzle 31 = which=20 delivers the working fluid, oil, into an oil supply chamber or = reservoir=20 32 of a low pressure tank 33 which may be bolted to = the=20 adjacent end cover plate 19 of the turbine, as indicated at = 34. The oil entering the reservoir chamber 32 = from=20 the exhaust stage of the turbine is at a pressure of about 3-5 = p.s.i.=20 In a second chamber 35 of the low pressure tank = 33=20 separated from the chamber 32 by an automatically moving or = self-adjusting free piston 36, compressed air at a = balancing=20 pressure of from 3-5 p.s.i. is maintained by a second pressure = regulating=20 valve 37. The pressure regulating valve 37 is = connected with the compressed air supply line 38 which = extends from=20 the regulating valve 11 to the high pressure chamber = 12 for=20 compressed air.

Within the chamber 32 is a gear = pump=20 39 or the like having its input shaft connected by a = coupling=20 40 with the turbine shaft 27. Suitable = reduction=20 gearing 41 for the pump may be provided internally, as = shown, or in=20 any other conventional manner, to gear down the rotational speed = derived=20 from the turbine shaft. The pump 39 is supplied with = the oil=20 in the filled chamber 32 delivered by the exhaust nozzle or = conduit=20 31 from the turbine. The pump, as illustrated, has = twin=20 outlet or delivery conduits 42 each having a back-pressure = check=20 valve 43 connected therein and each delivering a like = volume of=20 pressurised oil back to the high pressure chamber 15 at a = pressure=20 of about 500 p.s.i. The pump 39 also has twin fluid = inlets.=20 The pump employed is preferably of the type known on the = market as=20 "Hydreco Tandem Gear Pump," Model No. 151515, L12BL, or = equivalent. =20 In some models, other types of pumps could be employed including = pumps=20 having a single inlet and outlet. The illustrated pump will = operate=20 clockwise or counter-clockwise and will deliver 14.1 g.p.m. at = 1,800=20 r.p.m. and 1,500 p.s.i. Therefore, in the present = application of=20 the pump 39, it will be operating at considerably less than = capacity and will be under no undue stress.

=

Sinc= e=20 the pump depends for its supply of fluid on the delivery of oil at = low=20 pressure from the turbine 16 into the chamber 32, an = automatically operating by-pass sleeve valve device 44 for = oil is=20 provided as indicated in Fig.1, Fig.4 and Fig.5. = This=20 device comprises an exterior sleeve or tube 45 having one = end=20 directly rigidly secured as at 46 to the movable free = piston=20 36. This sleeve 45 is provided with slots = 47=20 intermediate its ends. A co-acting interior sleeve = 48=20 engages telescopically and slidably within the sleeve 45 = and has a=20 closed end wall 49 and ports or slots 50 = intermediate its=20 ends, as shown. The sleeve 48 communicates with one = of the=20 delivery conduits 42 by way of an elbow 51, and the = sleeve=20 48 is also connected with the adjacent end of the pump = 39,=20 as shown.

As long as the chamber 32 is filled with = low=20 pressure oil sufficient to balance the low air pressure in the = chamber=20 35 on the opposite side of free piston 36, such = piston will=20 be positioned as shown in Fig.1 and Fig.4 so that = the slots=20 47 and 50 of the two sleeves 45 and 48 = are out=20 of registration and therefore no flow path exists through them. = =20 Under such circumstances, the oil from the chamber 32 will = enter=20 the pump and will be delivered by the two conduits 42 at = the=20 required pressure to the chamber 15. Should the = supply of=20 oil from the turbine 16 to the chamber 32 diminish = so that=20 pump 39 might not be adequately supplied, then the = resulting drop=20 in pressure in the chamber 32 will cause the free piston = 36=20 to move to the left in Fig.1 and bring the slots 47 = into=20 registration or partial registration with the slots 50, as = depicted=20 in Fig.5. This will instantly establish a by-pass = for oil=20 from one conduit 42 back through the elbow 51 and = tubes=20 48 and 45 and their registering slots to the oil = chamber=20 32 to maintain this chamber filled and properly pressurised = at all=20 times. The by-pass arrangement is completely automatic and = responds=20 to a diminished supply of oil from the turbine into the chamber = 32,=20 so long as the required compressed air pressure of 3-5 p.s.i. is=20 maintained in the chamber 35.

Briefly, in summary, = the=20 system operates as follows. The pressurised inelastic and=20 non-compressible fluid, oil, from the chamber 15 is = throttled into=20 the turbine 16 by utilising the throttle valve 17 in = a=20 control station. The resulting rotation of the shaft = 27=20 produces the required mechanical energy or work to power a given=20 instrumentality, such as a propeller. A relatively small = component=20 of this work energy is utilised through the coupling 40 to drive = the pump=20 39 which maintains the necessary volumetric flow of oil = from the=20 turbine back into the high pressure chamber 15, with the = automatic=20 by-pass 44 coming into operation whenever needed. =

The=20 ultimate source of energy for the closed power system is the = compressed=20 elastic fluid, air, in the tank or bottle 10 which through the = regulating=20 valves 11 and 37 maintains a constant air pressure = in the=20 required degree in each of the chambers 12 and 35. = As=20 described, the air pressure in the high pressure chamber 12 = will be=20 approximately 500 p.s.i. and in the low pressure chamber 35 = will be=20 approximately 3-5 p.s.i.

It may be observed in = Fig.1 that=20 the tank 33 is enlarged relative to the tank 13 to=20 compensate for the space occupied by the pump and associated = components.=20 The usable volumes of the two tanks are approximately = equal.=20

In an operative embodiment of the invention, the two free = pistons=20 14 and 36 and the tank bores receiving them are 8 = inches in=20 diameter. The approximate diameters of the bladed turbine = wheels=20 are 18 inches. The pump 39 is approximately 10 = inches long=20 and 5 inches in diameter. The tank 13 is about 21 = inches=20 long between its crowned end walls. The tank 33 is = 10 inches=20 in diameter adjacent to the pump 39.

The terms and=20 expressions which have been employed herein are used as terms of=20 description and not of limitation, and there is no intention, in = the use=20 of such terms and expressions, of excluding any equivalents of the = features shown and described or portions thereof but it is = recognised that=20 various modifications are possible within the scope of the = invention=20 claimed.

The Clem = Engine.
This engine is based on an entirely different = principle,=20 and one which is not spoken about very often. Hurricanes or = =93twisters=94 as they are sometimes called, are large rotating = air masses of=20 incredible power which develop in hot areas which are more than = eight=20 degrees North or South of the equator. The distance from = the=20 equator is essential as the rotation of the Earth is needed to = give them=20 their initial spin. They usually develop over water which = is at a=20 temperature of twenty-eight degrees Centigrade or higher as that = allows=20 the air to absorb enough heat energy to get started. That = is why=20 there is a distinct =93hurricane season=94 in these areas, since = at certain=20 times of the year the ocean temperature is just not high enough to = trigger=20 a hurricane.

What is not generally realised is that a = hurricane=20 develops excess energy due to its swirling circular movement. = The=20 generation of this extra power was observed and documented by = Viktor=20 Schauberger of Austria, who also used his observations to great = effect.=20 I think that what Schauberger says makes some people = uncomfortable=20 as they seem to think that anything =93unorthodox=94 has to be = weird and too=20 peculiar to be mentioned. This is rather strange as all = that is=20 involved here is a simple observation of how our environment = actually=20 works. A hurricane is wider at the top than at the bottom = and this=20 concentrates power at the base of the swirling mass of air. = This=20 tapered rotation is called a =93vortex=94 which is just a simple = name to=20 describe the shape, but any mention of =93vortex power=94 (the = power at the=20 base of this rotation) seems to make many people uncomfortable = which is=20 most peculiar.

Leaving that aside, the question is =93can = we use=20 this energy gain from the environment for our own purposes?=94. = The=20 answer may well be =93Yes=94. Perhaps this principle is = utilised by=20 Richard Clem. In 1992, Richard Clem of Texas, demonstrated = a=20 self-powered engine of an unusual type. This engine, which = he had=20 been developing for twenty years or more, weighs about 200 pounds = (90=20 kilos) and generated a measured 350 horsepower continuously over = the full=20 period of a nine-day self-powered test. Although this = engine which=20 runs from 1,800 to 2,300 rpm is especially suited to powering an=20 electrical generator, Richard did install one in a car, and = estimated that=20 it would run for 150,000 miles without any need for attention and = without=20 any kind of fuel. Richard said that his prototype car had = reached a=20 speed of 105 mph. Just after receiving funding to produce = his=20 engine, Richard died suddenly and unexpectedly at about 48 years = of age,=20 the death certificate having =93heart attack=94 written on it as = the cause of=20 death. Remarkably convenient timing for the oil companies = who would=20 have lost major amounts of money through reduced fuel sales if = Richard=92s=20 motor had gone into production.

The motor is unusual in = that it is=20 a rotary turbine style design which runs at a temperature of=20 300⁰F (140⁰C) and because of that high = temperature,=20 uses cooking oil as its operational fluid, rather than water as = the oil=20 has a much higher boiling point. To a quick glance, this = looks like=20 an impossible device as it appears to be a purely mechanical = engine, which=20 will definitely have an operating efficiency which is less than = 100%.=20

In broad outline, the oil is pumped through a pipe and = into the=20 narrow end of the cone-shaped rotor. The engine is started = by being=20 rotated by an external starter motor until it reaches the speed at = which=20 it generates enough power to be sustain its own operation. = The=20 rapid spinning of the cone, causes the oil to run along spiral = grooves cut=20 in the inner face of the cone and exit through angled nozzles = placed at=20 the large end of the cone:

=

The = operating pressure produced by the pump is 300 to 500 psi. Richard = did not=20 attempt to patent his engine as US Patent 3,697,190 =93Truncated = Conical=20 Drag Pump=94 granted in 1972 as a liquid-asphalt pump is so close = in detail=20 that Richard felt that there was insufficient difference for him = to be=20 granted a patent:

Ther= e=20 appears to be considerable scope for anyone who wishes to build or = manufacture this engine and it is capable of acting as a heater as = well as=20 device for producing mechanical power. This suggests that = water=20 purification could be an additional =93extra=94 option for this = engine.=20

Prof. Alfred Evert of Germany has produced = an=20 analysis of the operation of the Clem Engine and turbines in this = general=20 category. His = website has=20 this to say:

07.05.=20 Centrifugal-Thrust-Engine=20

Objectives
Several different versions of = air-drive=20 engines have been described in the previous chapters. One = which is=20 particularly powerful, is the =93Suction-Cylinder-Engine=94 when = driven by=20 compressed air. Water-drive engines require a much more = complex=20 arrangement of closed circuits due to the strong centrifugal = forces caused=20 by using such a dense working-medium.

This new concept of = the=20 =93Centrifugal-Thrust-Engine=94 shows that centrifugal forces can = contribute=20 to turning momentum. Initially, however, we need to discuss = some=20 general points of view concerning the inertia of rotating systems. =

Gravity and Centrifugal Forces
First, = consider=20 the movement of a mass (a sphere or body of water) moving in a = circular=20 path around the inside wall of a hollow cylinder. = Centrifugal=20 forces always press radially outwards while Gravitational forces = always=20 act straight downwards. Fig 07.05.01 shows diagrams of three situations. A = partial plan=20 view of such a cylinder is shown in grey. This cylinder has = a=20 radius of 100 cm (R100). =20 Along its inner wall, mass M is=20 moving at a speed of 3.13 m/s (see arrow V3.13). This mass = is=20 continuously pushed inwards by the cylinder. This inward=20 acceleration A can = be=20 calculated by the formula Speed squared divided by Radius, in this case, with 3.13 m/s at a radius of 1 = m,=20 acceleration A =3D=20 (3.13)² / 1 =3D 9.8 m/s².

Matching= =20 that inward acceleration is the outward centrifugal force of that = mass.=20 That centrifugal force (A9.8) is shown as the red vector in the diagram. =20 Gravitational acceleration is also about 9.8 m/s², and = is shown=20 here as the green vector ( G9.8)=20 in the diagram, acting vertically downwards. The resulting = force is=20 shown as the blue line in the diagram. If the cylinder wall = were=20 replaced by the inside surface of a cone with a 45 degree = inclination,=20 then the mass would rotate at the same speed, maintaining a = constant=20 height.

Now, consider the middle diagram. Here, the = radius=20 distance to the wall is only 24 cm (R24) and the mass is only moving at 1.5 m/s (V1.5). The inward, = or=20 =93centripetal=94 acceleration produced is A =3D 1.52 / 0.24 which is 9.8 m/s2 so, here again, = the=20 centrifugal force (A9.8)=20 corresponds to acceleration under gravity (G9.8). = Consequently, the=20 diagram of the resolution of forces matches that of the previous = diagram.=20

So whenever a mass completes one rotation in exactly one = second,=20 the centripetal (inward) acceleration is the same as acceleration = under=20 gravity. At a radius of 1 m, the circumference is about = 3.13 m and=20 so the speed is about 3.13 m/s for one rotation per second. = At a=20 radius of 0.24 m, the circumference is about 1.5 m and so one = rotation per=20 second requires a speed of 1.5 m/s, and so identical results are = produced.=20 Whether this happens to be a pure coincidence or due to = some other=20 cause, is discussed later in the section entitled =93Aether = Physics=94.=20

In the lowest section of Fig = 07.05.01, a rotation at this same speed of 1.5 m/s (V1.5), but this time at = the shorter=20 radius of, say, 16 cm (R16)=20 produces a stronger inward acceleration given by A =3D 1.52 / 0.16 which = works out at=20 about 14 m/s². As the force diagram shows, this = results=20 in the mass rotating along a circular track which is higher up = than the=20 previous tracks. This can be seen in action when coffee in = a cup is=20 being stirred vigourously. =

Lifting-Force
Now=20 consider Fig 07.05.02 which=20 illustrates the effects of imposing higher rotational speeds on a = mass.=20 The radius of 24 cm (R24)=20 and of 16 cm (R16) = are now each=20 propelled at the higher rate of 6 m/s (V6). The inward =93centripetal=94 acceleration = is=20 correspondingly greater and is given by the equation A =3D 62 / = 0.24 which=20 works out at about 150 m/s² (A150) and about 225 m/s² (=20 A225 ) respectively.

In both = of=20 these cases, the centrifugal force is substantially greater than = the=20 gravitational force (shown as the short green near-vertical vector = marked=20 as G9.8) and so the = resulting=20 net forces (shown in blue in the diagram) are much closer to the=20 horizontal than before. These masses will therefore rotate = at a=20 constant height when moving along the inner face of a cone which = has much=20 steeper walls (shown in grey).

The lowest diagram of Fig 07.05.02 shows the = situation where=20 these forces press against a less steeply sloping wall (shown in = grey).=20 The wall resists this pressure by pressing back at right = angles to=20 its surface (dark green vectors). Consequently, the = remainder of=20 the nearly horizontal centrifugal force produces an upward = component=20 (H20 and H30, shown in red), = parallel to the=20 sloping face of the wall. Depending on the speed of the = mass and=20 the angle of inclination of the wall, this upward force causes an=20 acceleration of the mass, upwards along the wall. In these=20 examples, that acceleration is about 20 to 30 m/s². = In=20 our example of coffee being stirred in a cup, the faster the = stirring and=20 the more angled the sides of the cup, the larger the amount of = coffee=20 which spills over the lip of the cup. Notice that part of = this=20 centrifugal force becomes a component which acts in a direction = opposite=20 to gravity. In our example, the 6 m/s (six revolutions per second = or 360=20 rpm), produces a lifting-force which is much greater than the = force of=20 gravity.

Spiral Tracks
In Fig=20 07.05.03, the diagrams on the left hand = side show=20 sphere A, which = might be a=20 bowling ball, rolling in a straight line from right to left on a = flat,=20 horizontal surface. The plan view presented immediately = below,=20 shows that the movement of the sphere is a straight line. = However,=20 as shown at the bottom left of the Figure, if the sphere is = projected at=20 an angle, into a vertical cylinder, then it follows an upward = helical=20 track from E to = F in the diagram. = The path=20 followed is similar to a screw thread inside a nut or on the = outside of a=20 bolt. This same path would be followed if the moving object = were a=20 jet of water rather than a solid sphere.

The=20 corresponding three diagrams on the right hand side of Fig 07.05.03 show the = situation for=20 the sphere if instead of a vertical cylinder, it is projected into = an=20 inverted cone shape. In this instance, the path followed is = a=20 spiral curve starting at point K=20 and continuing to point L.=20 When this movement is shown on a flat surface, you will = notice that=20 the sphere rolls in a curve towards point D.

This shows clearly that there is an = additional=20 sideways force C = acting on the=20 sphere, causing this curved path. This has the effect that = when the=20 sphere is projected into the cone shape, it exits at point L with a greater upward = angle than=20 that with which it enters the cone at point K. This effect is also seen if a jet of water = is used=20 rather than a sphere or bowling ball. It should also be realised = that as=20 the sphere runs upwards along the inside surface of the cone, that = it=92s=20 path gets progressively steeper the further it rolls.=20

Steeper, Shorter and Faster
In Fig 07.05.04 the inner = surface of the=20 cone of Fig 07.05.03 = is shown=20 opened out to form a flat surface. The cross-lines shown = are=20 positioned to indicate each 30 degree strip of the conical = surface. =20 If a jet of water is projected into the lower edge of the cone at = point=20 A, at an angle of 30 = degrees,=20 then it will exit from the top of the cone at point B some 150 degrees later = (sector S150). The angle of = exit is=20 also 30 degrees and the spiral track C, shown in blue, is the path followed during it=92s = constant,=20 steady rise though the cone.

The = blue=20 line D shows what = happens when a=20 jet of water is projected into the cone. It enters the = lower edge=20 of the cone at an angle of 30 degrees as before, but this time the = water=20 velocity is greater. As a result of this higher velocity, = the water=20 now exits from the upper edge of the cone at a steeper angle of = about 35=20 degrees. That track D=20 runs within a sector of the cone which spans only 120 degrees = (S120) and so the track = followed is=20 shorter, steeper and covered more quickly than the jet of water = flowing=20 along the previous track C.=20

The diagram at the bottom right hand side of Fig 07.05.02, shows the = cone as seen=20 from the top. Track C=20 with its constant rate of rise is shown, as is the steeper and = shorter=20 track D. The = far side of=20 the cone, shows several paths which indicate how the water flows = if the=20 angle of entry at the bottom of the cone, is increased in steps.=20

The diagram at the bottom left shows the cross-sectional = view of=20 the section of cone used in this discussion. It shows how = the water=20 enters at the bottom edge, moves along the inner wall and exits = from the=20 upper edge of the cone. The vector M shows the diagonal thrust of the water against the = wall of=20 the cone. This is the direct equivalent of the two forces = G (against the wall) and = H (upwards along the = wall). =20 Force H is much = greater here=20 than with the earlier example where the rate of upward movement = was=20 constant.

Provisional Result
In this = first=20 section, only well-known facts have been mentioned. However, an=20 understanding of these examples and their points of view will be = important=20 during the following discussion:

We have noted that:=20

Centrifugal force equals that of gravity for one rotation = per=20 second.
A mass at this velocity maintains a constant height on a = wall=20 inclined at 45 degrees.
If the mass moves faster than that, it rises up the inner = wall.
The lifting force increases with increased velocity and/or = wall slop=20 and
The track along the inner wall surface becomes increasingly=20 steeper.
The mass moves with increasing speed as it progresses = towards the=20 outer edge of the cone.

The = =93Centrifugal-Thrust-Engine=94 is=20 based on the principle that a hollow cone-shaped cylinder is a = =91passive element=92. = Additionally, a=20 working medium flowing along it=92s stationary inner wall, is an = =91active element=92. These = key properties=20 are now discussed in the following section:=20

Rotor-Cylinder
Fig=20 07.05.05 shows a representation of a = turbine T. Initially, this = is shown as=20 a round cylinder. At the top left hand side of the diagram, = a=20 vertical cross-section is shown, and to the right of that is the = view from=20 above. The diagram at the bottom of the Figure shows the = inside=20 wall of the cylinder opened out and laid on a flat surface. = The=20 cylinder in this example has a radius of 16 cm (R16) and a circumference = of 1 metre.=20 Circular pipes are positioned vertically around the = circumference=20 to act in a similar way to turbine-blades (TS shown in blue). Here, twelve of these pipes = are shown,=20 each parallel to the system axis and running in a straight line = from=20 bottom to top.

A = 6 m/s jet=20 of water enters the bottom of these pipes at an upward angle of 30 = degrees. Due to the rotation of the cylinder drum, the = water moves=20 along the diagonal path A to=20 B. As = explained earlier,=20 the water has a horizontal velocity component marked in red in the = diagram=20 as V6, and because = of the angle=20 of entry of the water, there is a vertical speed of about 3.5 m/s = (shown=20 in green and marked as V3.5).=20 The water flowing in these pipes actually flows in a spiral = path=20 diagonally upwards, following the path shown by the blue line = running from=20 A to B. If the height of = the=20 cylinder is 24 cm (H24), then=20 the water moves around through the whole of sector S150 during its upward = flow through=20 the vertical pipes.

Rotor-Cone
At the top = left=20 hand side of Fig 07.05.06 a=20 conical cylinder turbine T is=20 shown. The pipes running up the inside of the cone are set = with a=20 16 cm radius at the lower edge of the cone (R16) and a 24 cm radius = (R24) at the top of the = cone. =20 These pipes therefore have a curved shape as they run up the = inside face=20 of the cone. These pipes can be thought of as performing = the same=20 function as turbine blades in a jet engine.

In the = same=20 way as before, a jet of water is fed at an upward angle of 30 = degrees into=20 the bottom of the pipes. Unlike the previous case, the jet = of water=20 does not strike the walls of the pipes at their lowest point = because the=20 water is entering parallel to a diagonal wall. In this = case, as=20 before, the overall height of the cylinder is 24 cm. The = track=20 taken by the water will be exactly the same as the previous track, = running=20 from A to B shown in the previous = diagram, and=20 again spanning a sector of 150 degrees (S150).

The central diagram of Fig=20 07.05.06 shows the conical cylinder = surface laid out=20 flat. The dark blue curve C shows the path taken by the jet of water as it = spirals=20 upwards and outwards from A to=20 B, within the sector = S150 shaded in blue. = =20 Interestingly, since the cone circumference at the outlet level is = longer=20 than at the inlet level (having 24 cm and 16 cm lengths = respectively), the=20 cone actually rotates at a greater speed than the speed of the = water.=20 This means that the water accelerates as it passes up = through the=20 curved pipes inside the cone (although that is not the intended = job of any=20 turbine).

As shown in the top right hand diagram, the = pipes inside=20 this conical turbine need to be curved backwards in the opposite = direction=20 to that in which the turbine rotates. These pipes are = curved to=20 follow the path shown in red and marked G which is contained within the 50 degree sector = S50.

As stated = earlier, the=20 water flowing in these pipes presses against the outer wall, due = to=20 centrifugal force. Once the water speed is great enough, = the water=20 gets lifted upwards by its own motion. If the pipes allow = that=20 additional upward motion, then the water will exit from the top of = the=20 pipes at a more acute angle than the angle of entry at the bottom = of the=20 pipes.

The bottom diagram shows a design arrangement where = the=20 water enters at an angle of 30 degrees (point E), and exits at the same = 30 degree=20 angle (at point F). = With=20 this arrangement, the water travels along a shorter, steeper path = D in a narrower sector of = just 120=20 degrees (S120). = Due to=20 this shorter path, the pipe follows a different curve, such as the = one=20 shown in red and marked H in the diagram. The pipe itself, = is=20 contained in a sector of just 40 degrees (S40).

The diagram at the top right hand side of = the=20 Figure, show this short pipe run. The water enters at point = A and flows upwards = through the pipe=20 marked G, to exit at = point B.

Notice that the = pipe curves=20 away from the direction of rotation. This is because the = pipe acts=20 something like a jet engine and the direction of thrust is in the = opposite=20 direction to the direction of the jet of water coming out of the = pipe.=20 The pipe shown in this illustration covers a sector of 50 = degrees.=20 However, remember that the water flowing in that pipe = covers a=20 sector of 150 degrees due to the rotation of the turbine cone. = The=20 lower pipe H shows = the other=20 design and it spans just 40 degrees. Water in that pipe = flows=20 upwards from E to = F and passes through 120 = degrees due=20 to the rotation of the turbine cone, and it also flows faster and = reaches=20 its outlet earlier. These different pipes are only shown on = a=20 single turbine cone for illustration purposes, as any turbine = construction=20 will have all of its pipes constructed to one design or the other = and not=20 a mix of the two shapes. =

Turbine-Blades
On=20 the left hand side of Figure = 07.05.07, shown in red, is the =91neutral=92 track H of the actual water flow = when=20 crossing a cylindrical sector of 40 degrees (S40). Also shown in = the top=20 left hand diagram, (shown in dark blue) is the corresponding steep = track=20 D followed by the = water when it=20 flows across a cylindrical sector of 120 degrees (S120). In the lower = left hand=20 diagram, the corresponding paths for the flows across a conical = turbine=20 surface are shown.

However,= if=20 the flowing water is to be used to generate a driving force on the = turbine=20 cylinder or cone, then the diagrams on the right hand side of the = Figure=20 show the necessary arrangement. To achieve this aim, the = pipes=20 carrying the water need to be curved to a greater degree. = Here, the=20 curve of the pipes is increased by, say, an arbitrary additional = 50=20 degrees to give a total of 90 degrees, as indicated by the curves = marked=20 L (shown in red) = within sector=20 S90. =

Correspondingly,=20 track K (shown in = blue) is=20 curved more sharply upwards with its sector reduced to a width of = just 70=20 degrees (S70). = This=20 amount is the previous 120 degrees, reduced by our arbitrary 50 = degrees.=20 The upper right hand side diagram shows the design for a=20 cylindrical turbine while the diagram below it shows the design = for a=20 conical turbine. The thin lines H and D = show the=20 original curves which would not apply any turning force to the = turbine=20 pipes were the water to flow through them. These paths = could be=20 called the =91neutral=92 tracks as they do not impart any thrust, = and it takes=20 the greater curvature shown by the thick lines to actually drive = the=20 turbine.

Cone-Wall and = Cone-Turbine
The lower=20 section of Fig 07.05.08 shows=20 the cross-section of turbine T=20 which has a radius of 24 cm (R24) at its upper edge and a radius of 16 cm (R16) at its lower edge and = which has a=20 height of about 24 cm (H24).=20 Below the main conical turbine (shown below the dotted = line) there=20 is an inlet section marked as TE=20 and which has an additional height of 12 cm (H12), and which tapers = down to a=20 radius of 12 cm (R12).

In the=20 previous example, the general arrangement of the turbine-blades = TS (shown in red), being = curved pipes=20 inside the turbine, was discussed. In this example, grooves = are=20 formed in the outer surface of the turbine cone. These = grooves, or=20 indentations, are open on the outside and the turbine cone is = housed=20 inside a cylindrical outer housing shown in grey and designated as = KW. This outer wall = supports an=20 inner conical housing (not shown) and the turbine rotor revolves = inside=20 that conical housing. Water (shown as light blue) fills the = space=20 between the turbine rotor and the outer conical housing. = The water=20 is bounded on one side by the smooth wall of the outer housing and = on the=20 other by the saw tooth shaped vertical grooves which form the = turbine=20 =93blades=94.

This example is needed to explain the = curvature of the=20 grooves at the surface of the cone. Unlike standard = turbines, the=20 water flows from a short radius inlet, to a much larger radius = outlet.=20 Water can=92t accelerate to reach the greater speed needed = at the=20 longer radius, so normal turbines have the water flowing from the = longer=20 radius inward towards the shorter radius. This causes = deceleration=20 of the water flow to generate torque. Consequently, our = design here=20 appears =91wrong=92 in conventional terms, and seems to make no = sense in=20 normal applications. This =91wrong=92 design only makes = sense when=20 using a cone-like rotor with its saw tooth-like blades.=20

Sawtooth-Blades
Mechanical turning = momentum=20 (torque) is generated by flows which press against one side of the = turbine=20 blades. Commonly, turbines have blades where a groove is=20 effectively created between two successive blades. In = effect, the=20 driving pressure of a turbine is applied to one face of this = virtual=20 groove. With this arrangement, the leading face represents = the=20 =93pressure=94 side and the trailing face represents the = =93suction=94 side.=20 The generation of torque is based on the difference of = pressure=20 between these two wall faces. This pressure difference is = maximised=20 if there is no suction side at all, that is, when there is no = pressure at=20 all on the =93suction=94 side. This is possible along the = surfaces of a=20 cone-shaped turbine which has saw tooth-like grooves as already = described.=20

These turbine =93blades=94 have a pressure-side which = faces in a=20 radial direction relative to the direction of rotation. = Each groove=20 has a =91bottom=92 or inner side which faces in a tangential = direction. =20 Water flow which moves diagonally outwards effectively flows = parallel to=20 that inner face. The pressure-side plus the inner-side, = form the=20 contours of an asymmetric saw tooth shaped groove. Each = inner-side=20 extends from the inner edge of the pressure-side to the outer edge = of the=20 following pressure-side. These triangular shaped grooves=20 effectively have no backside wall.

In Fig=20 07.05.08, the cross-sectional view shows = several=20 axial levels marked with the dotted lines A to H. = The=20 plan-view diagram shown at the top of the Figure indicates where = these=20 levels extend horizontally. At inlet level A, the radius is 12 cm and = a=20 ring-shaped cross-sectional surface is available for water to = enter=20 between the round turbine face and the round cone-shaped wall of = the=20 housing (drawn here across a sector of 30 degrees). =

Further up,=20 these tooth-shaped blades extend further out of the surface of the = turbine=20 cone. At point B, the=20 inner edge still has a radius of nearly 12 cm, while the outer = edge=20 extends further out into the ring-shaped groove. Here for = example,=20 twelve turbine =93blades=94 are shown, and in the 60 degree sector = B, there are two of these = =93saw-teeth=94.=20

Level C = marks the=20 junction between the turbine-inlet area (TE) to the main body of the turbine (T). The turbine = =93teeth=94 at this=20 level have a radius of 16 cm and this level has the deepest = grooves.=20 This sector of 60 degrees has two of these teeth TS.

Further up, = the outer=20 circumference becomes greater and the notches become longer. = If the=20 cross-sectional area for water flow were to remain constant, then = the=20 notches would need to be correspondingly shallower. In = sectors=20 D, E and F, which again span a 60 = degree=20 sector, two turbine-blades are shown in each sector.

As = sector=20 H covers only 30 = degrees, it=20 contains just one tooth. At this top level, which has a = radius of=20 24 cm, is located the turbine outlet, where water should exit, = forming a=20 homogenous flat jet. Consequently, the contours of the = turbine=20 rotor grooves should be ring-shaped. Also, the water which = previous=20 ran along the inner side of a cone-shaped wall, now is contained = in a=20 space between that wall and the inner turbine cone. These = surfaces=20 can effectively be a nozzle and this long groove can have = additional=20 divider walls (shown as thick red lines), to enlarge the = pressure-surfaces=20 in this area.

Winding Staircase
Fig 07.05.09 attempts to = give the=20 impression of the spiral arrangement of the previously described=20 tooth-shaped notches running around the surface of the turbine = cone.=20 The cone-like mountain shape has faces A running all around it. = These=20 faces start at a low angle and then become steeper as they rise = higher.=20 Each of these has a vertical wall B alongside it, formed by the side of the next = innermost face.=20 These faces are not visible at the right hand side of the = diagram=20 as their downward slopes are hidden from view.

For=20 clarity, in this diagram the cone is shown inverted, and so the = direction=20 of rotation appears clockwise, but in reality, when in its correct = position, the rotation will be counter-clockwise. Notice in = the=20 upper diagram, that the incoming water D hits these faces at nearly a right-angle, providing = substantial thrust in the direction of the arrows.

As the = lower=20 diagram shows the top view of the inverted cone it has the = appearance of a=20 conical hill. At points E and=20 F, lines are marked = which=20 indicate the height of the saw tooth shaped indentations in the = surface of=20 the cone. The lines at E=20 represent the pressure-side, while at F the inner side indicates only the slope surface and = thus no=20 =91suction-side=92 exists.

Now these indentations are not = arranged to=20 run straight down but are shifted as shown in the diagram at point = G. Previous = vertical=20 indentations E now = create the=20 pressure-wall H, = which=20 corresponds to the previous indentation A in its spiral path. The inner-walls F of the earlier = indentations thus=20 create the surface M = through=20 their vertical walls B. =20 In effect, the whole hill is built from these successive = =91winding=20 staircases=92, which admittedly actually don=92t have any steps. = These=20 paths spiral upwards with progressively smaller radius and = increasing=20 steepness.

At point N in=20 the diagram, part of several of these spiral pathways is shown. = =20 Here, the vertical walls between them are visible only as small = blue=20 curves. The whole of the surface area of this turbine cone = is a=20 pressure-side because of these spiral surfaces running all around = it.=20 Like diagonally falling rain, water flows all around the = surfaces=20 of that hill in its downward flow, and anywhere it is forced to = turn right=20 it generates a rotational force on the turbine cone. = Remember that=20 this machine has a cone-shaped housing which ensures that the = water flows=20 exactly in its intended path.

Crossing=20 Flows
To summarise, in Fig=20 07.05.10 the complete 360 degree surface = of the cone=20 is shown four times one below the other. Since the wide = part of the=20 cone has a radius of 24 cm it has a circumference of about 150 cm = (R24 and U150), while the narrow = part has a=20 radius of 16 cm and hence a circumference of about 100 cm (R16 and U100). The length = of the=20 side-surface is about 24 cm (H24). Using this example with these dimensions, = the upward=20 flow is along the indentations in the cone and along the walls of = the=20 cone.

The = angle=20 of entry of the water at the narrow circumference was assumed to = be 30=20 degrees. Maintaining this steady angle would cause the = water flow=20 to cover an angular sector of about 150 degrees, exiting at that = same=20 angle. Due to the centrifugal force of water striking the = wall at=20 an angle, an upward force is generated which causes the water to = follow a=20 steeper track and exit after crossing a sector which spans only = 120=20 degrees or so (S120) = and exit at=20 an increased angle of about 35 degrees. That track D (drawn in blue) is shown = several=20 times in the top diagram.

Water flowing in indentations = will=20 follow this track. However, this water can=92t follow the = faster=20 moving wider circumference at the top of the cone. In order = to=20 achieve the =91neutral-force=92 track for the complete path across = the cone,=20 the indentations need to have an increased backward curvature of = one=20 third. This indentation track H is shown in red and is contained within a sector of = 40=20 degrees (S40) and = this path is=20 also drawn several times in the top diagram.

In order to = have the=20 turbine generate a mechanical turning force, the indentations need = to be=20 curved backwards more strongly. Here, for example, that = sector was=20 extended to cover 90 degrees (S90) so water is channelled outwards faster, and exits = after=20 covering only 70 degrees (S70).=20 In the second diagram that indentation L (shown in red) and = water=20 track K (shown in = blue) are=20 drawn several times.

The indentations of the turbine are = shown=20 here as saw tooth-like notches which are open on their outer side. = =20 This arrangement results in two separate flows: on the one hand, = there is=20 forced flow within the indentations and on the other hand there is = the=20 free flow of water on the wall of the cone. In the third = diagram,=20 these indentations L = (shown in=20 red) are drawn several times as are the tracks of the free-flowing = water=20 D (shown in blue). = These=20 two paths cross each other at an angle of about 90 degrees.=20

Because free-flowing water projected upwards is too slow = for the=20 turbine-surface which is moving rather fast, but the water = movement will=20 be fast enough if it flows along the indentations L which are curved = backwards as shown=20 in the bottom diagram. In this diagram, both track D (shown in blue) taken by = the=20 free-flowing water and the indentation-forced track K (shown in red) are = shown. =20 Again, both flows are drawn several times and it can be seen = clearly that=20 these paths cross each other at an acute angle. The = free-flowing=20 water =91brushes=92 across the water which is flowing forwards in = the=20 indentations. It does this in the direction of rotation and = this=20 causes the water flowing in the indentations to start revolving.=20

Water within the indentations becomes redirected backwards = and=20 transfers it=92s inertia to the pressure-sides of the = indentations, thus=20 decelerating it=92s forward motion. This water still has = centrifugal=20 force, but the further out it progresses, the faster the = pressure-sides=20 run away ahead of it. This water which is flowing =91too = slowly=92 can=20 only apply pressure to the walls if they were much more strongly = curved=20 backwards, and even in that case it would only be by a small angle = which=20 would impart practically no additional turning momentum. =

Also,=20 free-flowing water can=92t keep up with the faster movement of the = turbine=20 at its larger exit circumference. However, the outward = water flow=20 is easily fast enough to fill the grooves with water and produce=20 additional rotation around its longitudinal axis. This=20 revolving-water-cylinder effectively works like a gear wheel as it = applies=20 the pressure of the free flowing water on to the pressure-sides of = the=20 grooves. The water flowing along the cone-wall is not = pressed into=20 the grooves, and so it is not redirected and its forward motion is = not=20 decelerated. So the centrifugal forces of that free-flowing = water=20 can go on contributing to the turning momentum of the turbine, but = only=20 indirectly, by driving that water-cylinder within the grooves.=20

Spin inside the Grooves
Fig 07.05.11 shows = sections of the=20 area between the cone wall KW (shown in grey) and the turbine cone = T. Free-flowing = water moves=20 alongside the cone wall, moving upwards and outwards. At = the=20 surface of the turbine, the turbine blades TS (light shading) are arranged in the shape of saw = tooth-like=20 notches. Water flowing within these grooves is guided = outwards=20 along the ever steepening track. Turning momentum is = generated by=20 the redirection of this part of the water flow.

On the=20 pressure-sides of these grooves, there is also the additional = pressure of=20 the free flowing water B. =20 This component of the water flows along a path which is not so = steep and=20 so it moves faster in the direction of rotation, i.e. it sweeps = over the=20 grooves. This generates a revolving movement C, in the water flowing = inside the=20 grooves. This increases the pressure on the pressure-sides = of the=20 grooves. So, this free-flowing component of the water flow, = contributes=20 indirectly to the turning momentum of the turbine.

The = diagram at=20 the lower left hand side of the Figure is a sketch of the outlet = at the=20 top of the turbine. The inner wall of the cone is curved = slightly=20 inwards as shown. This guides the free-flowing component of = the=20 water flow into the grooves. It should also be noted that = as this=20 part of the water is redirected, it is also decelerated which = contributes=20 further to the turning momentum of the turbine.

At the = lower right=20 hand side of the Figure, both the cross-sectional and longitudinal = views=20 of the outlet are shown. Here, the groove is no longer saw=20 tooth-like but instead it has a constant width, and this causes = the water=20 to exit in a continuous jet. The groove here is rather wide = and=20 could well be divided by the introduction of additional blades = ZS, which would allow the = water=20 pressure to be applied to a greater surface area.

To = summarise;=20 with this arrangement, not all of the water flow is forced into = the=20 grooves and immediately redirected and decelerated. The=20 free-flowing parts of the water are allowed to move in its natural = direction and under the influence of the centrifugal forces they = follow a=20 steeper path as they flow outwards and upwards. Moving = along this=20 track causes the water to cross over the water flowing in the = grooves.=20 This in turn, causes the water in the grooves to rotate as = it flows=20 upwards and this additional revolving movement add to the torque = being=20 generated by the water flow. Finally, as it nears the = outlet, the=20 free-flowing component of the water is directed into the grooves = and this=20 redirection causes a deceleration which adds even further to the=20 rotational drive of the turbine.

One further beneficial = effect=20 which is easily overlooked, is the fact that the water in each = groove=20 forms a long stretch of rotating water. This length of = rotating=20 water rotates faster in the upper sections of the groove and a = twisting=20 vortex of this type generates a strong suction which pulls the = water=20 entering the turbine inlet, strongly upwards towards the outlet of = the=20 turbine. This has been described in detail in earlier = chapters and=20 is further discussed later on in this document.=20

Cross-Sectional Surfaces
The lower = diagram of=20 Figure 07.05.12 = shows a=20 cross-sectional view through a cone-shaped turbine T, which has it=92s intake = extended=20 downwards by an additional section TE. Between the turbine and the conical wall = KW (shown in grey), water = flows from=20 the intake at the bottom E and=20 exits at the upper outlet A.=20 This flow has two components. The first, which is = shown in=20 dark blue, flows freely along the conical wall. The second, = which=20 is shown in light blue, flows in the grooves or indentations = formed by the=20 saw tooth-like turbine =93blades=94.

The = upper=20 diagram in the Figure shows a schematic cross-sectional = representation of=20 the plan view of this turbine. The ring-shaped water outlet = A is shown in light-blue. = This=20 outlet is formed between the inside of the conical housing, which = has a 24=20 cm radius at this level, and the cone which has a 22 cm radius. = =20 These are marked as R24 and=20 R22 respectively, = and between=20 them a 2 cm wide outlet is formed, with a cross-sectional surface = area of=20 about 290 cm² (F250).=20 Also shown in light blue, is the ring-shaped inlet E, formed between a radius = of 16 cm=20 and one of 12 cm (R16 and R12), and so is 4 cm wide, = with a=20 cross-sectional area of about 350 cm² (F350).

On the = right hand side=20 of the Figure is shown the previous curve D (shown in dark blue), which represents the track of = the water=20 flowing in the grooves. Water enters the turbine along its = lower=20 edge, at an angle of about 30 degrees and exits from the top of = the=20 turbine at an angle of about 60 degrees. Free-flowing water = also=20 enters the underside of the turbine at a very low angle and flows = upwards=20 until near the outlet it is directed into the grooves where it = also exits=20 the turbine at that same steep angle.

In the example = above, it was=20 assumed that the inlet water speed was about 7 m/s (V7), i.e. = entering at=20 an angle of 30 degrees while moving in the horizontal direction at = about 6=20 m/s (V6), the same = speed that=20 the turbine is moving at that level. The inlet, water has a = vertical rate of movement of about 3.5 m/s (V3.5). If we were = to assume=20 that the water speed at the outlet is also 7 m/s, due to it=92s = steep exit=20 angle of 60 degrees, it=92s horizontal velocity will be only 3.5 = m/s. =20 However, it actually exits at a vertical speed of 6 m/s (see the=20 vector-graphs).

Within pipes, the linear speed of flow is=20 inversely proportional to the cross-sectional area of the pipe. = In=20 our particular case, due to the rotational component of motion, = the flow=20 also depends on the =91gradient=92 of the flows, and not just the = speed of=20 movement in the axial direction. If water exits at the top = at 6 m/s=20 through an opening with a cross-sectional area of 250 = cm², then=20 if the inlet flow has a vertical speed of only 3.5 m/s, then it = would=20 require an inlet cross-sectional area of about 430 cm², = so our=20 cross-sectional area of only 390 cm² is a little too = small.=20

Suction Effect through Centrifugal = Force
It=20 was mentioned above, that centripetal (inward) acceleration is = stronger=20 than the acceleration under gravity at relatively low speeds = within a=20 radius as narrow as this. Since centrifugal force increases = with=20 the square of the speed, the outward pressure is a multiple of the = weight=20 of the water. With the inclination of the conical housing = wall=20 shown here, about one third of this force results in an upward = push along=20 that wall.

Because of this, the upward water flow gets = shifted on=20 to an increasingly steeper track and consequently it exits from = the=20 turbine outlet at a rather acute angle. But if the = cross-sectional=20 area of the intake is too small, then a sufficient mass of water = is=20 prevented from flowing into the turbine and the upward movement is = hindered. This causes the free-flowing component of the = water to=20 move along a flatter track, which again results in increased = centrifugal=20 forces. So, finally, an inlet with too small a = cross-sectional area=20 creates enormous suction forces and the inlet water is pulled = upwards very=20 strongly.

The turbines described in previous chapters, = could only=20 use the flows generated by pumps. With an air-driven = machine, it is=20 possible to generate areas of relative void into which air = particles move=20 through their own normal molecular movements. Autonomous=20 acceleration up to the speed of sound is possible with a minimum = of input=20 energy. Water is not compressible, so pressure is = transmitted=20 through water immediately. Suction pressure also acts = immediately=20 with no delay. Consequently, if the water in the upper = areas of the=20 turbine is pushed upwards by centrifugal forces, these forces also = exert=20 an upward pull on the water lower down in the turbine. So = unlike=20 all of the machines described earlier, in this turbine, flows are=20 generated based on the effects of centrifugal force alone. =20 Experiments with similar machines has confirmed that more water = was pulled=20 upwards than gravity would have been able to move downwards when = acting on=20 the same mass of water, even when just simple cones with plane = surfaces=20 were used.

Pump-Turbine = Hybrid
Turbines of=20 this type can also work as a pump. If the cone is driven = around,=20 then it will cause the surrounding water to rotate. At the=20 housing=92s conical wall, water gets lifted through the = centrifugal force.=20 That =91pump=92 has no forward-facing surfaces and so it = can=92t affect=20 the pressure. The water is presented with vertical walls in = close=20 proximity to =91winding staircases=92 which move continuously = dragging the=20 water into rotation. The higher that the water is lifted, = the=20 greater the cone radius encountered, and the greater the = centrifugal=20 forces which it experiences.

As the rotational motion = increases,=20 the lifting force-component become stronger and the water gets = pressed=20 into the diagonal surfaces of the grooves, and the turning = momentum is=20 achieved which allows the pump to become self-powering and no = longer=20 needing any input power to continue operating. If the speed = of=20 rotation continues increasing, and turbine-mode is achieved, then, = if the=20 turbine is not loaded it will accelerate automatically until the = water=20 can=92t enter the inlet any faster or alternatively, until the = turbine=20 self-destructs.

Safety first: Avoiding=20 Liability
In Figure = 07.05.13, the previous discussed elements are shown = installed in=20 housing G (shown in = grey) along=20 with some additional elements. The most important new = component is=20 the =91sluice-valve=92 B (shown in=20 yellow). This is a ring-shaped device which can be raised = or=20 lowered (as shown on the right hand side of the diagram), to = control the=20 water flow, and if necessary, bring the device to a complete = standstill in=20 the event of uncontrolled self-acceleration.

If=20 preferred, that control valve can be of different construction and = installed elsewhere. A definite requirement of any piece of = equipment of this type is the ability to guarantee complete safety = during=20 operation. It should be remembered that centrifugal forces = increase=20 with the square of the speed, which means that the rapid rotation = of a=20 mass of just one kilogram can generate a loading on the housing = wall of=20 several tons. Part of this enormously enlarged force is = converted=20 into turning momentum.

I have only = described=20 movement principles in general, and how some constructional = elements could=20 be designed. However, it must be made completely clear, = that I=20 accept no responsibility or liability for the actual construction = or use=20 of any such machines. The complete responsibility for all = risks,=20 rests solely with whoever decides to actually construct or operate = any=20 such machine. =

Circuit
As described in detail above, water (shown in light = blue) is=20 sucked in through inlet E<= /FONT>= <= /FONT>= <= /FONT>= <= /FONT>= <= /FONT>= <= /FONT>= <= /FONT>= <= /FONT>

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