ES2342582A1 - Procedure for the utilization of the casimir force. (Machine-translation by Google Translate, not legally binding) - Google Patents
Procedure for the utilization of the casimir force. (Machine-translation by Google Translate, not legally binding) Download PDFInfo
- Publication number
- ES2342582A1 ES2342582A1 ES200700363A ES200700363A ES2342582A1 ES 2342582 A1 ES2342582 A1 ES 2342582A1 ES 200700363 A ES200700363 A ES 200700363A ES 200700363 A ES200700363 A ES 200700363A ES 2342582 A1 ES2342582 A1 ES 2342582A1
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- Spain
- Prior art keywords
- procedure
- plates
- casimir force
- movement
- parallel
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- 238000000034 method Methods 0.000 title claims abstract description 10
- 239000002184 metal Substances 0.000 claims abstract description 6
- 239000011248 coating agent Substances 0.000 claims description 2
- 238000000576 coating method Methods 0.000 claims description 2
- 206010040925 Skin striae Diseases 0.000 claims 3
- 208000031439 Striae Distensae Diseases 0.000 claims 3
- 230000003100 immobilizing effect Effects 0.000 claims 1
- 210000001577 neostriatum Anatomy 0.000 claims 1
- 230000000694 effects Effects 0.000 abstract description 4
- 238000006073 displacement reaction Methods 0.000 abstract description 2
- 238000000926 separation method Methods 0.000 description 6
- 238000010276 construction Methods 0.000 description 1
- 238000012937 correction Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
Classifications
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- 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
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
- H02N11/00—Generators or motors not provided for elsewhere; Alleged perpetua mobilia obtained by electric or magnetic means
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- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Current-Collector Devices For Electrically Propelled Vehicles (AREA)
- Crushing And Grinding (AREA)
Abstract
Description
Procedimiento para la utilización de la fuerza de Casimir.Procedure for the use of force from Casimir.
La presente invención se refiere a un procedimiento que permite la construcción de motores utilizando el efecto Casimir.The present invention relates to a procedure that allows the construction of engines using the Casimir effect
Existen descripciones, alguna de ellas patentada, de dispositivos que permitirían obtener energía utilizando el efecto Casimir. Ninguno de ellos se ha construido jamás y, en cualquier caso, ninguno tiene nada que ver con el procedimiento que aquí se propone, salvo por la utilización del fenómeno físico mencionado.There are descriptions, some of them patented, of devices that would allow to obtain energy using the Casimir effect. None of them have been built never and in any case, none has anything to do with it procedure proposed here, except for the use of mentioned physical phenomenon.
En la Figura 1 se representa la sección transversal de dos láminas metálicas paralelas, A y B. La fuerza de Casimir, F, entre estas láminas varía inversamente con la cuarta potencia de la distancia que las separa. Se ha medido a distancias del orden de 1 \mu m y menores. Si la lámina B permanece fija y se restringe el movimiento de la lámina A, de modo que sólo pueda moverse en la dirección de la flecha, la componente F_{L} de la fuerza de Casimir causará el desplazamiento de la lámina A en dicha dirección.Figure 1 shows the section transverse of two parallel metal sheets, A and B. The force of Casimir, F, between these sheets varies inversely with the fourth power of the distance that separates them. It has been measured at distances of the order of 1 µm and less. If sheet B remains fixed and it restricts the movement of the sheet A, so that it can only move in the direction of the arrow, the component F_ {L} of the Casimir force will cause the displacement of the sheet A in said address.
En la Figura 2 se representan, en sección transversal, dos láminas metálicas, o con un recubrimiento metálico en las caras enfrentadas. Dichas caras enfrentadas presentan un ranurado triangular, en virtud del cual tenemos una situación como la descrita en la Figura 1, pero multiplicada. El efecto, en cualquier caso, sería el deslizamiento de la lámina A en la dirección indicada por la flecha, si B permanece fija y A sólo puede moverse en dicha dirección. Las redes de difracción que se construyen en la actualidad, aunque con criterios de planaridad más exigentes, serían una buena realización de las láminas que estamos describiendo. Parámetros normales de dichas redes son un ángulo W = 6º y una densidad de ranuras N = 1.200/mm. La inversa de N sería la longitud L que aparece en la Figura 2. Los cálculos realizados en condiciones ideales, es decir, sin aplicar correcciones, irrelevantes aquí, muestran que la componente de la fuerza sobre la lámina A en la dirección del movimiento, y causa del mismo, vale, por cada centímetro cuadrado de lámina, 1,64 dinas si la separación D vale 100 nm, descendiendo a 0,23 dinas por centímetro cuadrado si se duplica la separación y a 0,025 dinas por centímetro cuadrado si se cuadruplica (D = 400 nm).In Figure 2 they are represented, in section transversal, two metallic sheets, or with a metallic coating on the faces facing each other. These facing faces have a triangular grooving, under which we have a situation like the one described in Figure 1, but multiplied. The effect, in in any case, it would be the sliding of the sheet A in the direction indicated by the arrow, if B remains fixed and A can only move in that direction. The diffraction networks that are they build today, although with more planarity criteria demanding, would be a good realization of the sheets that we are describing Normal parameters of these networks are an angle W = 6º and a groove density N = 1,200 / mm. The inverse of N would be the L length shown in Figure 2. The calculations made in ideal conditions, that is, without applying corrections, irrelevant here, show that the force component on the sheet A in the direction of movement, and cause of it, okay, for every square centimeter of sheet, 1.64 dynes if the separation D is worth 100 nm, falling to 0.23 dynes per square centimeter if the separation is doubled and at 0.025 dynes per square centimeter if quadruples (D = 400 nm).
Los resultados que acabo de exponer permiten la realización de dispositivos que aportan una fuerza (o un momento) de manera continua, es decir, la realización de motores.The results I have just presented allow the realization of devices that provide a force (or a moment) of continuous way, that is, the realization of engines.
En la Figura 3 se representan dos discos metálicos enfrentados. Uno de ellos, el de la derecha, está fijo. El de la izquierda puede girar libremente alrededor de su eje. Las caras enfrentadas, según se aprecia en el detalle, están ranuradas radialmente. Este ranurado es, naturalmente, de paso decreciente a medida que nos vamos aproximando al centro de los discos. De lo anteriormente expuesto deducimos la generación de un par, dirigido sobre el eje del disco móvil, cuyo valor dependerá de los parámetros del ranurado, de su extensión en cada disco y de la separación de los discos. Para unos discos de lcm de radio, ranurados a 6º a partir de 0,5 cm desde el eje, de modo que sea N = 1,200/mm en el borde del disco (cuando el radio vale 1 cm) y N = 2.400/mm cuando el radio vale 0,5 cm, el par proporcionado vale alrededor de 0,4 din.cm si la separación entre los discos es 200 nm, reduciéndose unas siete veces cuando la separación se duplica.In Figure 3 two disks are represented metal faced. One of them, the one on the right, is fixed. He from the left you can freely rotate around its axis. The facing faces, as seen in the detail, are grooved radially This grooving is, of course, of decreasing step to As we approach the center of the discs. Of what above we deduce the generation of a pair, directed on the axis of the mobile disk, whose value will depend on the parameters of the grooving, its extension in each disk and the separation of the discs. For lcm radio discs, grooved at 6º to from 0.5 cm from the axis, so that it is N = 1,200 / mm in the edge of the disc (when the radius is worth 1 cm) and N = 2,400 / mm when the radius is worth 0.5 cm, the torque provided is worth around 0.4 din.cm if the separation between the disks is 200 nm, reducing about seven times when the separation is doubled.
En la Figura 4 se representan, en sección transversal, dos cilindros metálicos uecos concéntricos, fijo el exterior, pudiendo girar libremente el interior alrededor de su eje.In Figure 4 they are represented, in section transverse, two concentric uecos metal cylinders, fixed the exterior, being able to freely rotate the interior around its axis.
Las superficies enfrentadas, es decir, la interna del exterior y la externa del interior, están ranuradas en dirección perpendicular al dibujo, es decir, en la dirección del eje de los cilindros, según se ve en el detalle. Esta configuración aportará un momento al eje móvil que dependerá de los parámetros del ranurado, de la separación de las superficies enfrentadas, del área de dichas superficies y, por último, del radio de los cilindros. Es fácil obtener una estimación de su valor.The facing surfaces, that is, the internal external and external internal, are grooved in direction perpendicular to the drawing, that is, in the direction of the axis of the cylinders, as seen in the detail. This configuration will contribute a moment to the mobile axis that will depend on the parameters of the grooved, of the separation of the facing surfaces, of the area of said surfaces and, finally, of the radius of the cylinders. Is Easy to get an estimate of its value.
Claims (5)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
ES200700363A ES2342582B1 (en) | 2007-02-10 | 2007-02-10 | PROCEDURE FOR THE USE OF THE FORCE OF CASIMIR. |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
ES200700363A ES2342582B1 (en) | 2007-02-10 | 2007-02-10 | PROCEDURE FOR THE USE OF THE FORCE OF CASIMIR. |
Publications (2)
Publication Number | Publication Date |
---|---|
ES2342582A1 true ES2342582A1 (en) | 2010-07-08 |
ES2342582B1 ES2342582B1 (en) | 2011-04-25 |
Family
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
ES200700363A Expired - Fee Related ES2342582B1 (en) | 2007-02-10 | 2007-02-10 | PROCEDURE FOR THE USE OF THE FORCE OF CASIMIR. |
Country Status (1)
Country | Link |
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ES (1) | ES2342582B1 (en) |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5731361A (en) * | 1980-07-31 | 1982-02-19 | Eiichi Kikuchi | Rotary electric machine with magnetic force prime mover |
FR2586147A1 (en) * | 1985-08-07 | 1987-02-13 | Macheda Carmelo | Variable-speed vaned magnetic motor |
DE19525559A1 (en) * | 1995-07-13 | 1997-01-16 | Carl Fink | Perpetual motion drive arrangement - using drive-wheel with permanent magnets spaced on either side facing non-rotatable plates capable of moving in and out and each provided with spaced permanent magnets |
DE19629397A1 (en) * | 1996-07-20 | 1998-12-24 | Twelenkamp Joachim | Inclined magnet positioning method for electric motor or generator |
US6477028B1 (en) * | 1999-05-25 | 2002-11-05 | Fabrizio Pinto | Method and apparatus for energy extraction |
JP2004197727A (en) * | 2002-12-18 | 2004-07-15 | Isao Kajisa | Generator using casimir power such that two metal plates parallelly placed in slightly spaced relation in vacuum attract each other |
-
2007
- 2007-02-10 ES ES200700363A patent/ES2342582B1/en not_active Expired - Fee Related
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5731361A (en) * | 1980-07-31 | 1982-02-19 | Eiichi Kikuchi | Rotary electric machine with magnetic force prime mover |
FR2586147A1 (en) * | 1985-08-07 | 1987-02-13 | Macheda Carmelo | Variable-speed vaned magnetic motor |
DE19525559A1 (en) * | 1995-07-13 | 1997-01-16 | Carl Fink | Perpetual motion drive arrangement - using drive-wheel with permanent magnets spaced on either side facing non-rotatable plates capable of moving in and out and each provided with spaced permanent magnets |
DE19629397A1 (en) * | 1996-07-20 | 1998-12-24 | Twelenkamp Joachim | Inclined magnet positioning method for electric motor or generator |
US6477028B1 (en) * | 1999-05-25 | 2002-11-05 | Fabrizio Pinto | Method and apparatus for energy extraction |
JP2004197727A (en) * | 2002-12-18 | 2004-07-15 | Isao Kajisa | Generator using casimir power such that two metal plates parallelly placed in slightly spaced relation in vacuum attract each other |
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Publication number | Publication date |
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ES2342582B1 (en) | 2011-04-25 |
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