The current invention relates mechanical movement. More particularly the current invention relates to a system for moving a resilient member.
The human race has long sought different means by which to produce mechanical movement without employing manual labor. Domestication of animals was one of the earliest labor savings techniques to produce mechanical movement. This was followed by harnessing the wind to grind meal and move ships. This was followed by the use of steam, coal, crude oil and electricity by which to power an engine and move vehicles.
There is a need, therefore, to produce new techniques to generate mechanical movement.
In accordance with embodiments, there are provided systems and method for generating mechanical movement that includes a resilient member having an original shape. A bulwark is connected to the resilient member. A system is provided to selectively apply a torsional force to the resilient member using capillary forces to rotate the resilient member with respect to the bulwark. This places the resilient member in a deformed shape. The system also selectively terminates the capillary forces allowing the resilient member to return to the original shape. These and other embodiments are described more fully below.
Referring to
Referring to both
A supply 46 of fluid 48 includes an egress 50 positioned to deposit a portion 52 of fluid 48 into volume 44, using any known techniques to create a flow through egress, e.g., positive pressure applied to volume supply 46. The viscosity of portion 52 and dimensions of volume 44 are established so that upon application of portion 52, to one or both surfaces 33 and 42, capillary action occurs pulling surface 33 and 42 closer together, reducing the distance therebetween. Body 40 may be coupled with respect to bulwark 26 so that a distance between axis 28 and surface 42 may be controlled. With this configuration, the capillary action results in the movement of surface 33 toward surface 42. This is believed to occur as a result of intermolecular forces between the molecules of portion 52 and surfaces 33 and 42 that subjects resilient member 24 to a torsional force τ, which is in a direction away from body 40.
Torsional force τ1 causes twisting of resilient member 24 about axis 28, deforming resilient member 24. Deformation of resilient member 24 produces a restoring force FR in accordance with Hooke's law and which is in a direction away from surface 42. After completion of rotational movement, resilient member 24 is in a deformed state. In the deformed state, restoring force FR and torsional force τ are substantially at equilibrium, i.e. no further movement of resilient member 24 occurs. In this manner, resilient member 24 stores potential energy.
The potential energy stored in resilient member 24 may be released by disturbing the aforementioned equilibrium. This may be achieved in any convenient manner. For example, a mechanical force may be applied to body 40 causing a distance between body 40 and axis 28 to increase, i.e., applying a pulling force FP that moves in a direction away from body 40. Pulling force FP is of sufficient strength to overcome the intermolecular forces that exist between portion 52 and surface 33 and 42, referred to as release of intermolecular force, i.e., release. Specifically, the combination of restoring force FR and pulling force FP acting in opposite directions disrupts the aforementioned equilibrium and degrades the capillary action of portion 52. In response, resilient member 24 returns to the original shape by undergoing rotation about longitudinal axis 28. Resilient member 24 produces kinetic energy as it transforms between the deformed shape to the original shape. Upon reaching the original shape, resilient member 24 ceases rotating and once again defines volume 44, at which point both the potential energy and kinetic energy of resilient member 24 returns to zero. With restoring force FR and pulling force FP operating synergistically to terminate torsional force τ; it is not necessary that pulling force FP have a magnitude that is commensurate with either restoring force FR or torsional force τ. Pulling force FP need only be sufficient to disrupt the equilibrium that exists when restoring force FR is produced in response to resilient member 24 being subjected to torsional force τ. In one example, pulling force FP is applied manually with the use of one or more levers (not shown) that may be attached to either resilient member 24 and/or body 40.
Referring to
The magnitude of the capillary action provided by portion 52 is directly related to the 52 number of surface interactions between the molecules included in portion 50 and surfaces 42 and 33. To that end, it is desired that spacing 61 and depth 63 be established with respect to the size of molecules in portion 52 to provide rapid capillary action when surface 42 is disposed proximate to surface 33, with the exact dimensions being dependent upon the desired rate of capillary action. One example, provide spacing 61 and depth 63 with dimensions on the order of tens of nanometers to several 100 nanometers with the molecules in portion having dimensions smaller that either spaced 61 and/or depth 63. Additionally, portion have very low viscosity to provide rapid filling of volume 44, which includes recessions 51. An example of a low viscosity fluid is formed from isobornyl acrylate (IBOA) and n-hexyl acrylate (n-HA). An example of a composition of portion 52 comprises approximately 70 to 75% IBOA and 25-30% n-HA by weight which is believed to provide a viscosity in a range 2 to 10 Centipoises.
In an alternate configuration shown in
Referring to both
Referring to
Referring to both
Angle α is established so that upon restoring force FR1 and torsional force τ1 reaching equilibrium a second volume 244 is generated between a surface 119 of detent 118 and surface 142, which is in juxtaposition with and spaced-apart therefrom. The dimensions of volume 244 are established so that capillary action may occur between a second portion 152 of fluid 48 deposited therein and surfaces 119 and 142. This produces a second torsional force τ2. It is desired that second torsional force τ2 be greater than first restoring force FR1 in order to increase deformation of resilient member 24 and, therefore, increase the potential energy stored therein. To that end volume 244 is established to be greater than volume 144. For a given fluid 48 this may be achieved by providing greater areas of surfaces 119 and 142 that are in juxtaposition, when compared to the areas of surfaces 42 and 117. Alternatively, volumes 144 and 244 may have common dimensions and the portions of fluid 48 therein may be different fluids so that one which produces greater intermolecular forces with surfaces 142 and 199. To that end, egress 50 and/or supply 46 may be configured to move with respect to resilient member 34 and deposit fluid 48 in different volumes 144, 244, 344 and 444. As shown, supply 46 includes a second egress 152 positioned to deposit a portion of fluid 48, as described. In response to being subjected to torsional force τ2, resilient member 42 undergoes further deformation increasing the restoring force, referred to as a second restoring force FR2. Deformation, and therefore movement, of resilient member 42 ceases upon torsional force τ2 and second restoring force FR2 reaching equilibrium.
Angle β is established so that upon second restoring force FR2 and second torsional force τ2 reaching equilibrium a second volume 344 is generated between a surface 121 of detent 120 and surface 242, which is in juxtaposition with and spaced-apart therefrom. The dimensions of volume 344 are established so that capillary action may occur between a second portion 252 of fluid 48 deposited therein and surfaces 121 and 242 to produce a third torsional force τ3. It is desired that third torsional force τ3 be greater than second restoring force FR2 in order to increase deformation of resilient member 24 and, therefore, increase the potential energy stored therein. To that end volume 344 is established to be greater than volume 244, which may be achieved as discussed above with respect to volumes 144 and 244. In response to being subjected to third torsional force τ3, resilient member 42 undergoes further deformation increasing the restoring force, referred to as a third restoring force FR3. Deformation, and therefore movement, of resilient member 42 ceases upon third torsional force τ3 and third restoring force FR3 reaching equilibrium.
Angle γ is established so that upon third restoring force FR3 and third torsional force τ3 reaching equilibrium a fourth volume 444 is generated between a surface 123 of detent 122 and surface 342, which is in juxtaposition with and spaced-apart therefrom. The dimensions of fourth volume 444 are established so that capillary action may occur between a third portion 352 of fluid 48 deposited therein and surfaces 123 and 342 to produce a fourth torsional force τ4. It is desired that fourth torsional force τ4 be greater than third restoring force FR3 in order to increase deformation of resilient member 24 and, therefore, increase the potential energy stored therein. To that end, fourth volume 444 is established to be greater than third volume 344, which may be achieved as discussed above with respect to volumes 144 and 244. In the present example, supply 46 includes a fourth egress 352 positioned to deposit a portion of fluid 48 into fourth volume 444 to produce the capillary action described above with respect to volumes 144. In response to being subjected to fourth torsional force τ4, resilient member 42 undergoes further deformation increasing the restoring force, referred to as a fourth restoring force FR4. Deformation, and therefore movement, of resilient member 42 ceases upon fourth torsional force τ4 and fourth restoring force FR4 reaching equilibrium.
The potential energy stored in resilient member 24 may be released by disturbing the aforementioned equilibrium, as discussed above. For example, a mechanical force may be applied to any one of detents 40, 140, 240 and 340 to create pulling force FP that moves in a direction away from resilient member 24. It is desired that pulling force FP have sufficient magnitude to overcome the intermolecular forces present in any one of volumes 144, 244, 344 and 444. The combination of fourth restoring force FR4 and pulling force FP act in opposite directions to disrupt the aforementioned equilibrium and degrade the capillary action of one or the portions of fluids 48 deposited in volumes 144, 244, 344 and 444 when one or more detents 140, 240, 340 or 440 is subjected to pulling force FP. In one example, pulling force FP may act upon detent 440 that would result in the degradation of the intermolecular forces between portion 452 and surface 123 and 442. Considering that fourth restoring force FR4 is greater than any one of first torsional force τ1 second torsional force τ2 and third torsional force τ3, the kinetic energy produced by fourth restoring force FR4 would overcome the intermolecular forces in each of volumes 144, 244 and 344 to allow resilient member to return to the original shape.
The presence of intermolecular forces in volumes 144, 244 and 344 during release of molecular forces in volume 444 may result in attenuation of kinetic energy produced by resilient member 24. To reduce, if not avoid, these deleterious effects, it may be advantageous to release the intermolecular forces in one or more, and possibly all, of volumes 144, 244 and 344, before releasing intermolecular forces in volume 444. It is entirely possible that release of the intermolecular forces in one or more, and possibly all, of volumes 144, 244 and 344 may result in release of intermolecular forces in volume 444 before application of pulling force FP to detent 122. This may also result in attenuation of kinetic energy produced by resilient member 24 returning to the original shape. To avoid this situation one embodiment may include providing volume 444 with dimensions sufficient so that the intermolecular forces generated by portion 452 are of sufficient magnitude to maintain equilibrium with fourth restoring force FR4 in the absence of any one of first torsional force τ1, second torsional force τ2, and third torsional force τ3. In this configuration it is possible to release intermolecular forces in each of volumes 142, 142 and 342 while maintaining equilibrium with both restoring fourth force FR4 and of any one of fourth torsional force τ4. Thereafter, intermolecular forces in fourth volume 444 may be released by applying pulling force FP to detent 416.
It should be understood that the description recited above is list examples of the invention and that modifications and changes to the examples may be undertaken which are within the scope of the claimed invention. Therefore, the scope of the appended claims should be accorded the broadest interpretation so as to encompass all such modifications and similar arrangements, including a full scope of equivalents.
The present patent application claims priority to U.S. provisional patent application No. 61/147,470 entitled SYSTEM AND METHOD FOR MOVING A RESILIENT MEMBER, filed Jan. 26, 2009 and having Kenneth C. Brooks identified as an inventor, which is incorporated by reference herein in its entirety.
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Number | Date | Country | |
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20100193297 A1 | Aug 2010 | US |
Number | Date | Country | |
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61147470 | Jan 2009 | US |