GB2417307A - Gravity powered rotating engine - Google Patents
Gravity powered rotating engine Download PDFInfo
- Publication number
- GB2417307A GB2417307A GB0415330A GB0415330A GB2417307A GB 2417307 A GB2417307 A GB 2417307A GB 0415330 A GB0415330 A GB 0415330A GB 0415330 A GB0415330 A GB 0415330A GB 2417307 A GB2417307 A GB 2417307A
- Authority
- GB
- United Kingdom
- Prior art keywords
- ball
- loop
- energy
- arm
- rotation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03G—SPRING, WEIGHT, INERTIA OR LIKE MOTORS; MECHANICAL-POWER PRODUCING DEVICES OR MECHANISMS, NOT OTHERWISE PROVIDED FOR OR USING ENERGY SOURCES NOT OTHERWISE PROVIDED FOR
- F03G7/00—Mechanical-power-producing mechanisms, not otherwise provided for or using energy sources not otherwise provided for
- F03G7/10—Alleged perpetua mobilia
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- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Orthopedics, Nursing, And Contraception (AREA)
Abstract
An engine extracting gravitational energy from the movement of a ball includes a continuous loop spiralling unevenly along the axis 4 of a central shaft. As balls travel back and forth along the loops the device rotates about a central shaft. Gravitational energy is thus converted into mechanical energy.
Description
241 7307 :chik Motion Engine Lois indention is a zaichik motion engine
zmcbik motion ewe Mutely uses force of grayly to produce a rotational output on an axis point of its main sctwe. This is due to tlm ennnent wadis its =m strict which allows the constant Bee movement of its driven components Malls) and each lull gives an energy discharge into Me rotation of Me Much Woo each rotation.
A hip motion engine comprises of a number of Zeichilc motion arms file 1 imerconnected to item a zacllilc loop figure S. a number of balls 8 9, 10. 1 t, 12' a main ecus of radium 4 which lS bet g5 a = 25 which the bus Wed 6epeTkDt extends area.
A Field motion arm file 1 is m a tube form, which enables it to contain Ills The Cope of the motion aim such diet Me 411 gyrating its kinetic energy Mere is B Ion energy output into the arm "d win (be ball ' lo id kinetic energy there is a minims energy loss Gom Me This can be shown with Me three mam scions of the Idiom The first section of Me motion mm is We Why 1. Ibe straight enables We ball to fall m a Dear vertical manner fiom ball 12 to 11 to 9 which allows We hall geDR its =um kinetic energy as a result of We gravitational pull. The berth of the straight is equal to 11 distance at-rich the particular sloe and weight of a ball reach its no velocity. When the engine is an rotation Ring object does not start to generate its Icinetc until the straight of the mn passes its bonzonel 0-ee niggle. the point at which Me arm pa-eB 90 lees Cavity draws He driven aI:je down s- and He object has for effect on the movement of the The effect is minima} Hat the aim is nxwing downwards with the bell although the arm cannot move if than Me 11 as We nm speed movement ofthe arm Drill always be slower Wan Am speed of the driving objects. This is due to there always bed an element of resistance Ingest He rotation of the When the ball first starts its decest it is nut Acing in a vertical Erection but where Be Height of He and is venial the 11 meshed Is c=mn kinetic energy and Is moved a vertical direction, ball 9, This is due to Wl being coded within tube strait snd teas to foDow the direction of the s'bt and the gravitational you on the ball draws it down When the straight is Is vertical position He ball is at the end of He straight and moving in a cat direction al-, so to ll g the straight are synchronism m the wiiál pow n order to Move this timing can be altered ark 6 by almond He angle so that the ball 12 falls cerlier or later in the rotation Cow th: bell -1 the straight are syDchronisod the ball entry the em section 2 of the motion aim TO zig lion an Pled curve that has 2 main effects in relation to the xna] cube ofthe ball and also the movement of the structure When the HIS vertical lain-tic energy enters into the zai it pushes Us:zai away and as the zai section is Atwood to the Ritual anus point 4, He mowment away from the ball m rotation. The seventy of the eagle of He zap can be Stored to produce a differed finery tush into He rotation The greats He severity of He - 1 of the "i section the more innnedate the energy trfi is mto the rotation. Ibe longer or less severe the owe the greater the length of energy truer fiom the Wl but the Answer is less em:. 1-on the hovel of impact neccssa on n popular engulf akers the severe of the curve of He Pi seethe At the start of the 2:ai section tbe ball is moved vertically and at the end ofthe section the ball is mo horizontally. Throughout the zap section the All is in constant contact with the ann and u also constantly user the effects of gravity, iber^Te is coT-nt Ant relation hom gravity to 11 to An to rotation The amount of enterer traDsfared into He loop depends on weigh} of He AL The heavier He ball t more kinetic energy the 11 Awes =1 Refire Here is greacr energy mnsfi:r bled the rota.;,on Of the loop. The greater the weight of Me loop the Her energy Confer needs to be in order to Moper it and also any resistance against the Al of the Mop has to lie Counted for oath the elm Reefer through He zoo sectors, At the point which Be ball moving horizontally it 'inters into the row Action 3 of the motion ann The return section is a Radial spool. bank to the centre of the and also hack the start point of the next motion arm 11= echo Lion is Eyed n Caner that it does noT IT Me ban 10 Mom use its own kinetic energy to Wavy up Be also Be 11 does not preens retunt section firm using bs own kinetic energy from the Pi and Alcoa {let arm to move under the bale There me the Nan victors at Be start of Be reman Action The irk Rotor is Be movement of ball, which is mo at its maximum emetic end. If m was motionless at this pow driving o7adecm own lci-= energy would enable Be driven object to navel Ark up Lion to a chin point but not all Be way. I he An is travelling Into the dnnng object which the sewed factor it is also moving under Be ball nuked the Every distance of the Al led fir as Be bell is traYelli" over the An. He to the reman section mown up e ball and the ball moving over the aria He is en accumulative effect. The effect aLowst ball to travel Week to Be centre ofthe engine and uses a percentage of the energy, which ho earlier been ansf into rotation of Be em in the Zai-mm He third factor of the rennin section is the toppin eec:t of the 11. maul energy Aver n Agog tube arm under and driving tle bell over with a leYcl of diction to the arm At tba end of the return section of the Newton {be ball enters its next motion - in. He are rive main methods in which can be Thieved. Hey are Al over method tig= 4 and Frye and Be under anus method e3 figure 5. With the over method when Be hall nets to Be cerise of Be engine its hops and Eel up Ad over the point of ro - On, l1 8, and enters its new notion aim passed the YO-deee point of Be arm With the over mus method Me are two main proce$c which negatively effect We n=ven:ent of the engine. The first bed that ball goes against the Ion ul we engine when it skips is carried up and over Be poim of anus. Tlte second es Mat HI has a momentum vhich throws Be ball over the axis point and has a mild negative effect Eat Be rotation. '1 under meted does not have these reBatie effects agape Be radon, The ball 7 moves finely Hugh the central poicd: and is;nncdiately Be start of its next non arm urben it reaches Be centTe of the end. The type of method used also else he number of balls rotting within the engine.
With Be under His method the numb of balls determined lty the number of am and the angle At wash HI trawls espy Em. If 3 - d = is 20 deees pot its precious arm Mere is ago balls bomb within Be loop The emotion lior this is A. nb of) degrees past A+ (A*3hO) = B Dumber of balLs.
The Achy loop is balanced wheel and tam central poird of Cavity directly below the: point and due to Parr being the enterer Circe thy drives tle mine Trough balls situation of the balls nthln rotatme of the loop Is a iictor figure 5 and i igure 6. The Ham shows tbat the bans hew negative and a positive half with sieges ID a particular dir=mn ofthe lwp. With a loop Helling chlwme ball mown left ofthe con-1 axis has a negative elder OF the rotation as the Pop has to caky the 11 upwards. With Be elects of the 2:a a ball is propelled rigid the central point which maintains is mnyenent always into Me right side of Be engine which has 01 effcets on Be rotation of the loop. With the shape of return even aver the ball has lost its ohm lic energy the ball movement is mainlined relatively close to Be coal Bridal point Acts below the alas.
TO tome at Rich Be ball takes back energy Tom the Asian of the engine m Be Or - of the retune sections The effect Is minimal due to the Able of Be return but sIso the All is l closer to the cerise of Me Top which has a lesser enact Wan what it would posses if it was the out Inter. This is shown m figure 7 that denote a weight further away Bom central point of Bus has greater l on the central point Tan number otcqual weights closer to the central point and Be balance will tip to Be light.
The main energy prods by the engine is due to Be accumulation of after zap. Figure 5 shows a zuchik engme Bom a side view sad a fiontal Mew figure a. The side view elbows that with 7-arm model there is on Zen per 51+ degrees of rotation. A balls imiivillual Cleric em will allov it to pass several He's baby SIB taking some of as energy basic out of the rotation m effect a first 11 will allow several zag' of energy transfer to occur. At a pout there win tin when an ndidual ball closer to the con; rc of the loop will be in eyelet against Be enemy of Its tale Be ball will displace more energy;n the Lion of Be engine than He ball at talc Ice of the loop lewd on the sane principles of the balance theory displayed In figure 7. Another factor to this the shape of the return Section. As the emu n has no direct pup- He ball relation to the rotation Here is en umulmive movement emit between 11 md tbe loop. Tim distance generated the process leaves the lx 11 close to the centre ofthe enzyme, which ho a lesser effect on tho region of the loop than the l:'alt Tic "i 8 Cot eat on the roan wig a edc Try tensor Tom bell to Me at Each ball will tT&Yel down all He zaichilc alms wadis nuances of rotations and a sequence can tee shovel in figure S. Arm 1S is, the first ann and by Ravels to the next arm 17, Den lit end 21. The ball muses an do kin He bell needing, to ran back to she fim arm 15 to enclose and Item Chic loop. lithe ball Is Wok t firm ann15 fiom 21 to 20, then token 16 and 15.
If the loop is enclosed and the space between the bells is sealed I the bum bed a clow diameter of the tumid In there is a suction and compression eject been the b-, ball ttavell down the straight 22 slid zEn section will hew section effect on the Wl 23 previous Id a push eflbet on the ball 24 in li.ont Mown in figure 9. In ennment He balls hew to be tuned so Hat the pressure emit will wow with the rotation of He loop also so that He drib hall does not Use is ohm l'c energy es a consequence of the eject. With e correct timing of the driving ball and bum which An elf- this can uncrease the efficiency of the cogine' With a perforated tube dIbwing in in: freedom of of ad to outside of He tube will reduce this effect. Ike mavemcm of within (be tubing can bc diree so that there is a Covet of cool sir tbrouh the fitly engine sating at cipher side of the engine and fk through. Ibis can reglues an effect Am occur. With to mns-t contact of balls to loop time an alum of ilictn which oceans and a generation of hew which could damage Me eogire can be cnstffl. This can be reduced in a number of ways. The first is a cooling lubricate oil thst demises He tycoon as a lubricant and also nsinmin temperature within We caging. The second s We movement of sir through Ike Tic cwl'Dg it Aside and sri the tress Cough the air outside of to en,. In an echelon enYironrnent sl1 Me AT can be removed and therefore Otis less fffn and energy loss within the mchik loop. This could imp efficiency of He rooo of loop as me would be kits tffction and particles acting against He ball.
The ichik engine rotates Al a c04mcc of zai AL and the zei sections transfi;:ring awe Prosy ink the rotation than tlx rend balls use to rend to the centre and to: next zhik motion arm The rotonal mechanical energy prods can be Or ninny applies;w And one use Swell be to tuna a generator to produce an electrical output. Ci
Claims (17)
1. A Chick motion engine comprising a number of zachik notion Dins
interconnected to Elm a continuous loop with a number of balls rattling Withy die loop Ant create an energy transfer through the zai sections into a Station often;michi} loop.
2. The amid semmn of the I allows gravity to draw a ball downwards
3. The ball 12 tic I 1 to g generates more Antic energy the lordlier He strairt of the Seth but lass maximum Icinic energy
4. A baLI's kinetic energy is Hi into the Anton of the Hop Ash Ash Pi tbn of loop.
5. The greater the fi:equercy of the zai sections per rotation creates more energy transfer onto the 140p per rotatmm
6. The Hester the 11 greater the Irinete energy possessed by He ball and He He orgy transfer Into the rotation of the =elilc loop
7 The Are revue the zai section the none strop the energy transfer is fiom belI to rotation of the Pop but the shorter He alTunS oftime of He energy transfer
8. We 1 were ED and of the zap Sac less strong the energy transfer but the greater the amount of time of He erzeW tappet.
g. The We of the return section of the arm allows He ball to Abel mto flee rotation of loop.
10. The ball 10 allows the Cape of the reman sochon to travel under the
11.
I 1. We toppm effect of He ball when entering the return section has an eiSect ore propelling Be ball into over the return section.
12, Lee 1110 own kinetic energy and kinetic by of rotstn of lhe Cop takes tiu ball back to the cerise of the loop.
13. At the We of the engme the to figure ofthe ball entering He next arm can be altered enlace and 1sta by changing He angle of return in relation to He Text aT'm
14. The under effect figure 3 allows the ball to travel past the choral point of iledy and enter dirt into He next motion arm
15. Ire a sealed tube figure why a ball similar in dieter to He mbe, the saigl and zai ball will have suction effect on the boll previous to itoelfand a push effect on the ball Font as a oonsequere pull on the air behind and push of the aur in Ace.
16. Ike mbe In be perforated to allow air to travel through He engine cooling she engine caused by the Bastion of coinuo=; Use,
17. Temperature control lubricants can be usM to decrease the Bi&tion within the englac and mat- a cons eah win the loop 1 The loop can also be sealed and all air particles can be removed to Fume Edicts within the loop 19. The accumulation of zag aRM zag creates a meehcd rotational output of the zalchik loop connected to He exis point.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GBGB0316051.2A GB0316051D0 (en) | 2003-07-09 | 2003-07-09 | Zaichik |
Publications (2)
Publication Number | Publication Date |
---|---|
GB0415330D0 GB0415330D0 (en) | 2004-08-11 |
GB2417307A true GB2417307A (en) | 2006-02-22 |
Family
ID=27741856
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GBGB0316051.2A Ceased GB0316051D0 (en) | 2003-07-09 | 2003-07-09 | Zaichik |
GB0415330A Withdrawn GB2417307A (en) | 2003-07-09 | 2004-07-08 | Gravity powered rotating engine |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GBGB0316051.2A Ceased GB0316051D0 (en) | 2003-07-09 | 2003-07-09 | Zaichik |
Country Status (1)
Country | Link |
---|---|
GB (2) | GB0316051D0 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2012119483A1 (en) * | 2011-03-04 | 2012-09-13 | Wang Keren | Gravity transforming method |
WO2012119481A1 (en) * | 2011-03-04 | 2012-09-13 | Jin Lili | Method for achieving circular motion |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB332184A (en) * | 1930-01-15 | 1930-07-17 | John Goodwin | Self driving apparatus |
GB447737A (en) * | 1934-08-20 | 1935-03-06 | Thomas James Heskett | Power unit amplifier |
GB2040018A (en) * | 1978-05-30 | 1980-08-20 | Cowan D | Rotary device |
GB2044393A (en) * | 1978-12-14 | 1980-10-15 | Cambay E | Rotary Apparatus |
KR20010088605A (en) * | 2001-08-10 | 2001-09-28 | 이영한 | Perpetual Motion by YOUNG-HAN Theory |
-
2003
- 2003-07-09 GB GBGB0316051.2A patent/GB0316051D0/en not_active Ceased
-
2004
- 2004-07-08 GB GB0415330A patent/GB2417307A/en not_active Withdrawn
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB332184A (en) * | 1930-01-15 | 1930-07-17 | John Goodwin | Self driving apparatus |
GB447737A (en) * | 1934-08-20 | 1935-03-06 | Thomas James Heskett | Power unit amplifier |
GB2040018A (en) * | 1978-05-30 | 1980-08-20 | Cowan D | Rotary device |
GB2044393A (en) * | 1978-12-14 | 1980-10-15 | Cambay E | Rotary Apparatus |
KR20010088605A (en) * | 2001-08-10 | 2001-09-28 | 이영한 | Perpetual Motion by YOUNG-HAN Theory |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2012119483A1 (en) * | 2011-03-04 | 2012-09-13 | Wang Keren | Gravity transforming method |
WO2012119481A1 (en) * | 2011-03-04 | 2012-09-13 | Jin Lili | Method for achieving circular motion |
Also Published As
Publication number | Publication date |
---|---|
GB0415330D0 (en) | 2004-08-11 |
GB0316051D0 (en) | 2003-08-13 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
WAP | Application withdrawn, taken to be withdrawn or refused ** after publication under section 16(1) |