Impact detection system

Information

  • Patent Grant
  • 6392527
  • Patent Number
    6,392,527
  • Date Filed
    Wednesday, September 4, 1996
    28 years ago
  • Date Issued
    Tuesday, May 21, 2002
    22 years ago
Abstract
An acceleration change detection system, which in a preferred embodiment is used as an impact detection system, detects whether a deflection sensor is deflected. The magnitude and/or direction of the impact may be considered. The system may include one or more than one deflection sensor. The invention may have particular use in a system that determines whether to deploy an air bag in a vehicle. The system may employ an open or enclosed chassis. The deflection sensors may deflect against deflection structures, which may be in various shapes. The deflection sensors have an electrical parameter (such as resistance) that changes upon deflection of the deflection sensor. In certain embodiments, the deflection sensor is ordinarily held in place by a movement inhibitor, which may include, for example, a magnetic, spring, clip, or stiff substrate. A large impact may create a force great enough to overcome the magnetic or mechanical force of the movement inhibitor. Deflection sensors may be arranged to detect movement in the x, −x, y, −y, z, and −z directions. Electrical circuitry may produce a voltage that is indicative of the change in resistance, which in turn is indicative of the extent of deflection. The extent of deflection is an indication of the magnitude of the impact. Determining circuitry interprets changes in the electrical parameter(s) to determine information regarding the impact and, perhaps, trigger an air bag. The movement detection system also may be used to detect skidding or other movement of the vehicle.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The invention relates to an acceleration change detection system, which in a preferred embodiment is used as an impact detection system. More particularly, the invention relates to such a system that employs a deflection sensor. The invention may have particular use in a system that determines whether to deploy an air bag in a vehicle.




2. State of the Art




Detection of movement and forces has wide application. For example, automobile air bag systems employ accelerometers in determining whether to inflate the air bag.




Prior art detectors used in deploying air bags have included a cylinder in which a ball is ordinarily held in place by a magnet at one end of the cylinder. A spring is positioned at the other end of cylinder. The cylinder and the ball are gold plated to be electrically conductive. When the vehicle has a collision at the front, the vehicle including the cylinder rapidly decelerates. When there is sufficient force, the ball breaks loose from the magnet and travels toward the spring. Accordingly, the magnet is chosen to have enough magnetic force to hold the ball in place unless a threshold force is created through a collision. The threshold force varies depending on vehicle specifications.




When the ball strikes the spring, an electrical circuit is completed, causing a squib switch to be activated and in turn causing an explosion which inflates an air bag.




Disadvantages of the prior art detection system include that it detects an impact in only one direction and generally lacks flexibility of application.




Accordingly, there is a need for an impact detection system that will detect impact in various directions and has flexibility in applications.




SUMMARY OF THE INVENTION




An acceleration change detection system includes a deflection sensor having an electrical parameter that changes upon deflection of the deflection sensor. The deflection sensor may be a flexible potentiometer. The deflection sensor may be deflected against a deflection structure. The deflection structure may include any of a variety of shapes. A non-pivoting attachment may also facilitate deflection. The system may include a movement inhibitor that ordinarily prevents the deflection sensor from deflecting within a particular range of deflection, but that allows deflection within the particular range in response to sufficient change in acceleration of the movement inhibitor. Examples of a movement inhibitor include magnets, springs, and clips. A particularly stiff substrate of the deflection sensor may also inhibit movement.




Determining circuitry that is connected to the deflection sensor may generate a signal indicative of a value of the electrical parameter and determine whether the deflection sensor is deflecting within the particular range based on the indicative signal. The determining circuitry may respond to merely the presence of deflection, that the deflection exceeds a threshold, or to a particular value of a threshold. In each case, the deflection is within a range. The system may include air bag triggering circuitry for triggering an air bag.




The system may include more than one deflection sensor, each having an electrical parameter that changes upon deflection of the deflection sensor for detecting deflections in various directions. The deflection sensors may be joined in a group (for example, to a chassis and/or in a loop) or separated. The determining circuitry may generate signals indicative of values of electrical parameters of the additional deflection sensors, and determines whether the deflection sensors are deflecting within particular ranges based on the indicative signals. Vector mathematics may be used to determine a direction.




Deflection values may be stored for forensic purposes.











BRIEF DESCRIPTION OF THE DRAWINGS




While the specification concludes with claims particularly pointing out and distinctly claiming that which is regarded as the present invention, the advantages of this invention can be more readily ascertained from the following description of the invention when read in conjunction with the accompanying drawings in which:





FIG. 1A

is a partially schematic side view of one embodiment of an acceleration change detection system according to the present invention shown in the ordinary position.





FIG. 1B

is a partially schematic side view of the embodiment of

FIG. 1A

shown in an activated position.





FIG. 2A

is a partially schematic perspective view of another embodiment of an acceleration change detection system according to the present invention shown in the ordinary position.





FIG. 2B

is a partially schematic perspective view of the embodiment of

FIG. 2A

shown in an activated position.





FIG. 3A

is a partially schematic perspective view of another embodiment of an acceleration change detection system according to the present invention shown in the ordinary position.





FIG. 3B

is a partially schematic perspective view of the embodiment of

FIG. 3A

shown in an activated position.





FIG. 4A

is a partially schematic side view of another embodiment of an acceleration change detection system having multiple deflection sensors in ordinary positions.





FIG. 4B

is a top view of the system of FIG.


4


A.





FIG. 4C

is a side view of the system of

FIG. 4A

in an activated state.





FIG. 4D

is a top view of an alternative system of sensors that may be formed in a loop.





FIG. 5A

is a cross-sectional side view of a detection system that detects a significant change in acceleration in the z direction.





FIG. 5B

is a cross-sectional side view of a detection system that detects a significant change in acceleration in the −z direction.





FIG. 5C

is a cross-sectional side view of a detection system that detects a significant change in acceleration in the z and −z direction.





FIG. 5D

is a cross-sectional side view of a detection system that detects a significant change in acceleration in six directions.





FIG. 6

is a more detailed schematic block diagram representation of a portion of the system of

FIGS. 1A and 4A

.





FIG. 7A

is a side view of another alternative system in an ordinary state.





FIG. 7B

is a side view of the embodiment of

FIG. 7A

in an activated state.





FIG. 8A

is a cross-sectional view of another alternative system in an ordinary state.





FIG. 8B

is a cross-sectional view of the embodiment of

FIG. 8A

in an activated state.





FIG. 9A

is a side view of another alternative system in an ordinary state (shown in a solid line) and activated state (shown in a dashed line).





FIG. 9B

is a side view of another alternative system in an ordinary state (shown in a solid line) and activated states (shown in a dashed line).





FIG. 10A

is a side view of another alternative system in an ordinary state (shown in a solid line) and activated state (shown in a dashed line).





FIG. 10B

is a side view of another alternative system in an ordinary state (shown in a solid line) and activated state (shown in a dashed line).





FIG. 10C

is a side view of another alternative system in an ordinary state (shown in a solid line) and activated states (shown in a dashed line).





FIG. 10D

is a side view of another alternative system in an ordinary state.





FIG. 11A

is a side view of another alternative system in an ordinary state.





FIG. 11B

is a side view of the embodiment of

FIG. 11A

in an activated state.





FIG. 12

is a side view of an optical detection system.





FIG. 13

is a side view of a flexible potentiometer in various degrees of deflection.











DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS




Referring to

FIGS. 1A and 1B

, one embodiment of an acceleration change detection system


10


includes a flexible potentiometer


12


suspended from a support


14


. Various deflection sensors other than a flexible potentiometer may be used. Detection system


10


may detect a change in acceleration from zero acceleration (i.e. no speed or constant speed) to a positive acceleration or negative acceleration (also called a deceleration). Detection system


10


may detect a change in acceleration from one non-zero acceleration to a different non-zero acceleration. Acceleration change detection system


10


may be used as an impact detection system.




A flexible potentiometer has a resistance (which is an example of an electrical parameter) that changes as the flexible potentiometer is deflected. Details regarding flexible potentiometers are discussed below. The flexible potentiometer has a first portion


12


A and a second portion


12


B with the second portion


12


B deflecting relative to the first portion


12


A as shown in

FIGS. 1A and 1B

. The resistance of flexible potentiometer


12


changes as it is deflected about a deflection structure


16


as shown in FIG.


1


B. Deflection structure


16


is supported by a support


18


. Supports


14


and


18


may be part of or attached to any of various structural pieces of an automobile.




The value of the resistance (or other electrical parameter) is measured by determining circuitry


20


through conductors


22


A and


22


B. Determining circuitry


20


may determine an actual value of the electrical parameter or whether it, for example, merely exceeds a threshold. Triggering circuitry


24


may trigger various devices including, for example, a device to inflate an air bag and an anti-skid device.




As shown in the drawings, the deflection structure may be any of a variety of structures against which a deflection sensor may deflect.




A magnetic post


28


acts as a movement inhibitor to flexible potentiometer


12


to which a magnet


30


is attached. Magnetic post


28


and magnet


30


are examples of magnetic pieces. Ordinarily, the magnetic attraction between magnetic post


28


and magnet


30


is great enough to keep flexible potentiometer


12


from significantly deflecting about deflection structure


16


. As an example, support


14


, deflection structure


16


, and magnetic post


28


are traveling in the x direction and have a large deceleration (which is a negative acceleration). There is a tendency for magnet


30


and flexible potentiometer


12


to continue to travel in direction x. If the tendency is great enough, the magnetic attraction between magnetic post


28


and magnet


30


is overcome and flexible potentiometer


12


deflects about deflection structure


16


.




The flexibility of the substrate of flexible potentiometer


12


may vary. In some embodiments, the substrate may be so stiff that a movement inhibitor is not required.





FIGS. 2A and 2B

show another embodiment of an acceleration change detection system in which a flexible potentiometer


12


is ordinarily held in place by the attraction between magnetic pieces


34


and


36


, but deflects about deflection structure


16


in response to a great change in acceleration. In one embodiment of flexible potentiometer


12


, a variable resistive material


40


is deposited on a substrate between conductors


42


A and


42


B, which are connected to conductors


22


A and


22


B.





FIGS. 3A and 3B

show still another embodiment of an acceleration change detection system in which a spring


38


is a movement inhibitor. Flexible potentiometer


12


may be connected to spring


38


or merely rest against it.




Another embodiment of the invention is illustrated in

FIGS. 4A

,


4


B, and


4


C. Referring to

FIGS. 4A-4C

, an acceleration change detection system


44


includes an actuator


46


suspended by a cable


64


from a chassis


48


. Acceleration change detection system


44


may be used as an impact detection system. Actuator


46


is shown to be spherical, but may be various other shapes including cylindrical or rectangular solid. Actuator


46


is magnetic and ordinarily held in position by a magnetic post


52


. Actuator


46


may be very close to or touching magnetic post


52


.




Flexible deflection sensors


50


A,


50


B,


50


C (not shown in FIG.


4


A), and


50


D, which may be flexible potentiometers, are joined at the bottom to chassis


48


(but could be joined at the top or some other position). Chassis


48


includes deflection structures


54


A,


54


B (not shown), and


54


C (not shown), and


54


D. Deflection sensors


50


A,


50


B,


50


C, and


50


D have an electrical parameter (such as resistance) that changes when the deflection sensors


50


A,


50


B,


50


C, and


50


D are deflected. In the embodiment shown in

FIG. 4A

, deflection sensors


50


A,


50


B,


50


C, and


50


D would preferably experience the change in parameter only when deflected in the direction of a corresponding deflection structure. For example, deflection sensor


50


A would experience the change in parameter only when deflected in the direction of deflection structure


54


A. Optional restraining devices


58


A and


58


D prevent movement in the other direction. (Corresponding optional restraining devices


58


B and


58


C are not shown to avoid clutter.)




For convenience, the following nomenclature is used. The x direction is toward the front of the vehicle, and the −x direction is toward the rear of the vehicle. The y direction and −y direction are toward the driver side and passenger side of the vehicle, respectively. The z direction and −z direction are toward the top and bottom of the vehicle, respectively.




The vehicle (or other object) to which chassis


48


is connected may experience a sudden acceleration, perhaps because of a crash. In such a case, chassis


48


(including restraining devices


58


and magnetic post


52


) also experience the sudden acceleration. Depending on the circumstances, the acceleration may be positive in one or more directions and negative in one or more directions. Positive acceleration is an increase in speed in a given direction. Negative acceleration (also called deceleration) is a decrease in speed in a given direction.




For example, if a forward moving vehicle has a head on crash, there will be at least a negative acceleration (or deceleration) in the x direction. On the other hand, if a stationary vehicle or a vehicle traveling in reverse has a head on crash, there will be at least a positive acceleration in the −x direction. If a vehicle has a crash on the passenger side, there will ordinarily be at least a positive acceleration in the y direction.




As an example, referring to

FIG. 4C

, when the vehicle is quickly moving and has a head-on crash, chassis


48


experiences a large negative acceleration (or deceleration) in the x direction. However, actuator


46


may pivot about a connection point


60


of cable


64


and, therefore, has a tendency to remain moving at a constant speed. If the impact force is great enough, the magnetic force between actuator


46


and magnetic post


52


will be overcome. If the magnetic force is overcome, deflection sensor


50


A will be deflected about deflection structure


54


A, as shown in FIG.


4


C.




Deflection sensors


50


A,


50


B,


50


C, and


50


D are connected to determining circuitry


20


through conductors


66


A,


66


B,


66


C, and


66


D respectively. (Additional conductors may carry signals from other deflection sensors, discussed below.) As it is deflected, the parameter (such as resistance) of deflection sensor


50


A changes. The change is detected by determining circuitry


20


through conductor


66


A. Based on the change in the parameter, and perhaps some other conditions such as the speed of the vehicle, determining circuitry


20


determines whether and how to respond to the change. In the case where more than one deflection sensor is deflected, determining circuitry


20


may use vector mathematics to determine the direction of the movement and, thereby, the impact. In certain embodiments of the invention, different air bags may be deployed depending on the direction of the impact. For example, a side door air bag could be deployed in response to a side impact. Alternatively, multiple air bags could be deployed. Also, the system may detect which seats are occupied and not deploy air bags toward a seat to which no one is seated. The presence of some one in a seat may be detected through deflection of one or more flexible potentiometers in the base of an automobile seat and/or the back of an automobile seat.




Depending on its design, determining circuitry


20


may respond to any change in the parameter at all, or only to a change in the parameter that exceeds a threshold. In this respect, the impact may have to be sufficient to overcome both the magnetic force of magnet


52


and to cause a sufficient deflection in deflection sensor


50


A. Deflection sensor


50


A may include a stiff substrate that would tend to resist deflection. However, in some cases, unless there is some means (such as a clip or strong spring) for keeping deflection sensor


50


A stationary, it will move in response to various changes in the speed of the vehicle. Accordingly, in many cases, determining circuitry


20


will respond only when the change in parameter exceeds a threshold. In the case in which there is an external deflection structure, deflection sensors may or may not pivot at the point of connection of the deflection sensor to a support surface. In the case in which there is no external deflection structure, it is preferred that the deflection structures do not pivot at the point of connection to facilitate deflection.




Still referring to

FIG. 4C

, if the vehicle is stationary and is struck head on by a rapidly moving vehicle, chassis


48


(including post


52


) experiences an acceleration in the −x direction. Actuator


46


has a tendency to remain stationary. If the impact force is great enough, the magnetic force between actuator


46


and magnetic post


52


will be overcome and deflection sensor


50


A will be deflected about deflection structure


54


A by actuator


46


. Depending on the strength of the magnetic force, flexibility of deflection sensor


50


A, and programming of determining circuitry


20


, a stationary vehicle must be struck by another vehicle having great momentum to cause activation of air bag(s).




Deflection sensor


50


D may be unnecessary in a vehicle system that is not designed to activate an air bag(s) in response to a rear collision. However, deflection sensor


50


D may serve other purposes, such as determining the direction of a collision in combination with one or more of sensors


50


A,


50


B, and


50


C. Such information may be useful for forensic purposes.




Four or more flexible potentiometers


12


could be arranged each on the outside of a common deflection structure.





FIG. 4D

shows an alternative to the embodiments of

FIGS. 4A-4C

, in which eight deflection sensors


72


A-


72


H are employed. The substrates of such deflection sensors may form a cylindrical loop.




Chassis


48


is not necessary, although some sort of support structure is. An enclosed chassis may be useful in keeping dirt or other foreign particles from interfering with components of impact detection system


44


.




Various sensing systems could be used to detect acceleration in the z direction or a −z direction. For example, referring to

FIG. 5A

, a sensing system


80


includes an actuator


84


(shown in, for example, a spherical shape) that is supported by a deflection sensor


86


. Support structures


88


A,


88


B (not shown),


88


C (not shown), and


88


D are connected to the vehicle and prevent actuator


84


from moving substantially in a lateral direction. Deflection sensor


86


may have substantial rigidity so that it ordinarily is not substantially deflected. Sensing system


80


may also include a deflection sensor


94


positioned above actuator


84


(i e., in the z-direction). Deflection sensor


94


may have very little rigidity so that it is easily deflected. Deflection structures


96


and


98


are positioned near deflection sensors


86


and


94


.




Referring to

FIG. 5B

, when the vehicle rapidly rises, deflection sensors


86


and


94


, support structures


88


A and


88


D, and deflection structures


96


and


98


rise with the vehicle. However, as deflection sensor


86


rises, the weight of actuator


84


tends to deflect deflection sensor


86


about deflection structure


96


.




Referring to

FIG. 5C

, when the vehicle rapidly lowers, deflection sensors


86


and


94


, support structures


88


A and


88


D, and deflection structures


96


and


98


lower with the vehicle. However, as deflection sensor


94


lowers it is struck by actuator


84


, which momentarily remains stationary, and thereby deflects against deflection structure


98


.





FIG. 5D

shows an embodiment in which side support walls


88


are replaced by deflection sensors (e.g. deflection sensors


50


A and


50


D) to provide a system that detects in six directions (x, −x, y, −y, z, and −z). Deflection structures


100


A,


100


B (not shown),


100


C (not shown), and


100


D facilitate deflection of deflection sensors


50


A,


50


B (not shown),


50


C (not shown), and


50


D.





FIG. 6

shows details of an example of determining circuitry


20


. Referring to

FIG. 6

, in a preferred embodiment deflection sensor


50


A is a flexible potentiometer having a substrate


102


on which variable resistance material


40


is applied between conductors


104


A and


104


B. The relative proportions are not necessarily to scale. A power supply


106


(such as a constant voltage or constant current supply) causes a voltage drop across variable resistance material


40


between conductors


104


A and


104


B. The voltage drop is detected by voltage detection circuit


108


A, the output of which is supplied to an analog-to-digital converter (A/D)


112


A. A microprocessor and/or dedicated hardware circuitry


114


interprets the digital voltages to decide the extent of deflection if any. The magnitude of the deflection is related to the magnitude of the voltage. The magnitude of an impact may be related to the magnitude of the deflection. Alternatively, conductor


66


A may be supplied directly to A/D


112


A or directly to dedicated hardware circuitry


114


. Dedicated hardware circuitry


114


may be analog and/or digital.




The extent of deflection of additional deflection sensors may be determined through conductors


66


B . . .


66


N, voltage detection circuits


108


B . . .


108


N, and A/D


112


B . . .


112


N. As noted, depending on the design, voltage detection circuits


108


B . . .


108


N, and/or A/D


112


B . . .


112


N are not necessary to supply voltages to microprocessor and/or dedicated hardware


114


.




Where more than one deflection sensor is used, determining circuitry may use vector mathematics to determine a direction. An optional memory


116


is used to store data related to deflection for forensic purposes.




A look-up table or equation may be used. In developing the data for the look-up table or the equation, one could consider the force necessary to overcome the magnetic force, and the amount of force dissipated before the impact reached impact detection system


44


. Data could be gathered empirically through comparing the values of voltages on conductors


66


during various crashes. In short, various analyses could be used as well as various existing or yet to be obtained data.




It is not necessary to consider the absolute value or the change in resistance of variable resistance material


40


. Rather, the values or changes in values of voltages would be sufficient for most purposes.




A single voltage determining circuit and A/D could be used by switching between conductors


66


A,


66


B, . . .


66


N.




In a preferred embodiment, when the voltage or change in voltage exceeds a threshold, microprocessor or dedicated hardware


114


activates a driver


118


, which in turn may activate a squib to inflate an air bag. For example, if deflection sensor


50


A is deflected beyond a threshold, microprocessor


114


may activate a squib


122


thereby inflating an air bag


124


. Deflection of deflection sensor


50


B beyond a threshold may lead to activation of a squib


128


and inflation of a different air bag


130


(e.g. a side door air bag). Alternatively, both air bag


124


and


130


could be inflated in response to deflection of a single deflection sensor. Deflection of one or more deflection sensors could lead to the inflation of an air bag


134


. Deflection to a certain level could lead to activation of a first squib


136


, while deflection to a greater level could lead to activation of a second squib


138


, which causes a greater inflation of air bag


134


. Under one embodiment of the invention, squib


138


would have a greater amount of explosive than in squib


136


. Alternatively, or in addition, a sensor (such as a deflection sensor) in a seat could determine the weight of the person sitting in the seat. Squib


136


could be activated if a lighter person were sitting in the seat, while squib


138


could be activated if an heavier person were sitting in the seat. Still alternatively or in addition, the weight of the person or the amount of the deflection could control the timing of the inflation of the air bag.




Microprocessor or dedicated hardware


114


may build in a delay depending on the direction and/or magnitude of the impact. Microprocessor or dedicated hardware


114


may also factor in the presence and/or weight of a person who would be in the path of an air bag in determining whether or how much to inflate an air bag.




Other embodiments of detection systems include the following. In

FIGS. 7A and 7B

, deflection sensor


50


A supported by chassis


162


, is ordinarily held in place by a spring


154


of a system


156


. In response to a large change in acceleration, deflection sensor


50


A deflects about deflection structure


164


as shown in FIG.


7


B.




In

FIGS. 8A and 8B

, in a system


170


, an actuator


174


is supported by a spring


178


, which in turn is supported by chassis


180


. Optional springs


184


A and


184


D hold deflection sensors


50


A and


50


D in place. Deflection occurs because deflection sensors


50


A and


50


D are not allowed to pivot at their lower ends (whether or not springs


184


A and


184


D are used).





FIG. 9A

shows a deflection sensor


50


for which deflection is detected only in the direction shown in dashed lines.

FIG. 9B

shows a deflection sensor


190


that may deflect in two directions as shown in dashed lines. Deflection sensors that deflect in two directions are discussed below.





FIGS. 10A and 10B

show a deflection sensor


50


for which deflection in the z or −z directions is detected. The deflection is shown in dashed lines.

FIG. 10C

shows a deflection sensor


190


for which deflection in both the z and −z direction may be detected.

FIG. 10C

is like

FIG. 10D

except that springs


194


A and


194


B are used.




Deflection sensors


50


and


190


may include a particularly stiff substrate that inhibits movement. Various movement inhibitors could be used in addition. Also, the associated determining circuitry may require a large threshold. Since every substrate inhibits movement at least by a small amount, the stiffness of a substrate will not be referred to herein as a movement inhibitor.




As shown in

FIGS. 11A and 11B

, a clip


202


may act as a movement inhibitor to deflection sensor


50


. Again, if deflection sensor


50


is not allowed to pivot, it will deflect without a separate deflection structure. The structure that prevents pivoting may be through a deflection structure.




Depending on how a deflection sensor is configured, the parameter (e.g. resistance) of the deflection sensor may change in response to being deflected in only one direction or in both directions. If a deflection sensor responds to deflection in only one direction, it can change from an x to −x, y to −y, or z to −z direction by reversing the orientation of the deflection sensor.




The various features may be mixed and matched. For example, those impact detection systems illustrated herein that do not include chassis protrusions, magnets, or springs could include such features. The various embodiments show the many possibilities.




Referring to

FIG. 12

, an optical detection system


210


, such as a photodiode and detection or fibre optic, could be used to measure motion of a magnet or actuator.




Merely as one example, the magnitude of a force, such as is caused by a collision, could be determined as follows. First, measurements may be taken to determine how much force it takes to overcome the magnetic attraction between magnetic pieces. Measurements could also be made to determine how much force is required to deflect a particular deflection sensor by a particular amount. These could be in the form of a look up table or an equation. It may also have to be factored in how much force is absorbed by the body of the vehicle. This would vary depending on what part of the car is struck.




For example, assume that the force absorbed by the vehicle is F


A


, the force required to overcome the magnetic force is F


M


, and the force required to deflect a flexible potentiometer by x is force F


x


. The force of a collision F


C


would then be F


A


+F


M


+F


x


.




The force absorbed by vehicles may be gathered by vehicle manufacturers.




A variable resistance material (e.g. variable resistance material


40


in

FIGS. 2A and 2B

) is applied to a substrate to create a flexible potentiometer. Flexible potentiometers are marketed under the mark Bend Sensor™ by Flexpoint, Inc., 656 West 7250 South, Midvale, Utah, 84047, which is associated with inventor Gordon B. Langford. Deflection sensors, other than flexible potentiometers, may have another electrical parameter that is altered through deflection. The variable resistance material may be formed of an electrically conductive ink which predictably changes electrical resistance upon deflection or bending between a first configuration and a second configuration. Various types of phenolic resin materials are presently believed to be suitable for the variable resistance material. For example, a phenolic resin Formula 3609 that has been manufactured by Electronic Materials Corporation of America (EMCA-REMEX Products, Ablestik Electronic Materials & Adhesives), 160 Commerce Drive, Montgomeryville, Pa., 18936, has been found suitable in that it is elastically flexible or bendable for many thousands of cycles or bends.




The variable resistive material may be a two-part epoxy material, a thermoset adhesive, or a thermoplastic, all incorporating conductive material such as graphite or carbon. The variable resistance material may include a carbon ruthenium.




Merely examples, the substrate may be from about 0.005 to about 0.010 inches in thickness (although various other thicknesses may be acceptable); the variable resistive material may be from about 0.0003 to about 0.001 inches in thickness (although various other thicknesses may be acceptable).




To attach to a substrate, the variable resistance material may include a material which facilitates wetting, gluing, or sticking. The variable resistance material may include graphite in combination with a binder. The variable resistance material is preferably of the type which is applied to the substrate in liquid form and which in turn dries to a solid form.




The substrate may be constructed of various materials including various polymers, such as polyamide, polycarbonate, polyimide (Kapton), and polyester (Mylar), which may be thermoplastics.




A resistive grid or flexible potentiometer may be used to measure a degree or angle of deflection. The more the deflection, the less the resistance. With measurements, a relationship between the degree or angle of deflection and the resistance can be developed and used in software, that would be relatively simple to create.




Segmented constant resistance conductive material may be used in combination with a flexible potentiometer to reduce the resistance and help linearize changes in resistance. The segmented conductors may be made of silver, silver alloys, or other conductive metals, as well as conductive carbon-based compounds. The segmented conductors may be applied in a liquid form, or applied in a solid form which is pressed onto the variable resistance material. The conductivity of the segmented conductors remains essentially constant upon deflection. Therefore, the segmented conductors provide paths for electrical current that are in parallel with the path provided by the variable resistance material. The segmented conductors act as attenuators. It is believed that the segmented conductors may help to make the resistance versus load curve of a flexible potentiometer more linear. The segmented conductors may help make the resistance at a particular deflection configuration more consistently repetitive.




The variable resistance material may be spray painted, rolled, silk screened, or otherwise printed onto the substrate. The variable resistance material may be a solid which is pressed onto the substrate. A conductive substrate may be used. The substrate may be connected to a particular potential, such as ground. A non-conductive coating may be applied to the substrate.




It is believed but not known that as a flexible potentiometer (of some or all compositions), is deflected or bent, the variable resistance material cracks or deforms. That is, in some or all compositions, dried variable resistance material has a granular or crystalline-type structure which cracks or breaks upon deflection. As the variable resistance material deflects, the number of cracks and the space between them is believed to increase, thereby changing the electrical resistance in a predictable manner. The change can be measured upon application of suitable electrical signals.




Certain flexible potentiometers have a substantial change in resistance only when deflected in a first direction from a straight position, not when deflected in an opposite direction from a straight position. For example,

FIG. 13

shows a side view of a flexible potentiometer


220


at various degrees of deflection, denoted A, B, C, and D. Flexible potentiometer


220


is a flexible potentiometer having a substrate on which a layer of variable resistance material is applied. At deflection degree A, which is straight, flexible potentiometer


220


has a resistance R


A


. At deflection degree B, flexible potentiometer


220


has a resistance R


B


, which is substantially greater than resistance R


A


. At deflection degree B, the level of resistance R


B


is predictable and repeatable. At deflection degree C, flexible potentiometer


220


has a resistance R


C


, which is substantially greater than resistance R


B


and is predictable and repeatable. Accordingly, as the deflection changes from degree C to degree B, there is a predictable and repeatable decrease in resistance. However, at deflection degree D, in flexible potentiometer


220


, there may be only a small change in resistance from resistance R


A


.




Other flexible potentiometers change resistance in either direction from a straight position. There are various ways of constructing a deflection sensor that senses deflection in two directions from the straight position. Under a first construction, a first layer of variable resistance material is applied to one side of a substrate and a second layer of variable resistance material is applied to the other side of the substrate. The first layer is connected between a first set of conductors, and the second layer is connected to a second set of conductors. When the substrate (along with the variable resistance material) is deflected in a first direction, the resistance between the first set of conductors increases by a repeatable and predictable amount, and when the substrate is deflected in a second direction, the resistance between the second set of conductors decreases by a repeatable and predictable amount.




Under a second construction, a layer of antimony tin oxide is applied over a substrate (e.g. a Kapton substrate), and a layer of variable conductive material is applied to the layer of antimony tin oxide. An extra layer of carbon may be applied over the layer of variable conductive material. When the substrate is deflected in a first direction from the straight position, the resistance of the variable resistance material increases by a predictable and repeatable amount. When the substrate is deflected in a second direction from the straight position, the resistance of the variable resistance material decreases by a predictable and repeatable amount.




Under another technique, a layer of variable resistance material is applied to a single side of a substrate. The substrate is deflected to an initial setting so that the variable resistance material has an initial resistance value greater than that of the straight position. As the deflection of the substrate is increased from the initial setting, the resistance increases. As the deflection of the substrate is decreased from the initial setting, the resistance decreases. One end of the flexible potentiometer may be weighted and the deflection may be about a pivot point.




An impact detection system according to the present invention may be made with switches, such as a membrane switch rather than a deflection sensor. In a membrane switch, the amount of resistance decreases as the force against the switches increases.




As used in the claims, the term “connect,” “connectable,” or “connected to” are not necessarily limited to a direct connection. The context is useful in determining the intent.




The movement detection system also may be used to detect skidding or other movement of the vehicle or control anti-lock brakes, or other anti-skid mechanisms.




The term chassis is not intended to be restrictive but rather inclusive. Indeed, a chassis may be comprised of one or multiple parts.




Having thus described in detail preferred embodiments of the present invention, it is to be understood that the invention defined by the appended claims is not to be limited by particular details set forth in the above description as many apparent variations thereof are possible without departing from the spirit or scope thereof.



Claims
  • 1. An acceleration change detector comprising:a support; a deflection sensor suspended from said support and extending away therefrom, said deflection sensor being formed to have a first portion and a second portion each being positioned to extend away from said support and to extend at least in part along an axis in an at rest position, and said deflection sensor being formed to have said second portion deflectable relative to said first portion from said at rest position to a displaced position in which said second portion is deflected away from said axis upon application of an acceleration force to said support of a magnitude to displace said second portion from said at rest position to said displaced position, said second portion being deflectable about a deflection point between said first portion and said second portion, said first portion and said second portion each being formed of a flexible substrate with an electrically conductive material deposited to extend from said first portion onto said second portion, said electrically conductive material having an electrical resistance that undergoes an ascertainable change in electrical resistance upon deflection of the second portion about said deflection point from said at rest position to said displaced position; movement inhibitor means positioned proximate said deflection sensor to inhibit said second portion from deflecting from said at rest position to said displaced position until said acceleration force exceeds a threshold acceleration force; and a deflection structure against which said second portion of said deflection sensor deflects when urged to said displaced position upon application of said acceleration force above said threshold acceleration force to said support.
  • 2. The acceleration change detector of claim 1, further comprising determining circuitry that is connected to the deflection sensor to sense change in said electrical resistance of said electrically conductive material deposited on said substrate of said deflection sensor, said determining circuitry generating deflection signals indicative of said at rest position and said displaced position of said second portion.
  • 3. The acceleration change detector of claim 2, further comprising air bag triggering circuitry connected to said determining circuitry to receive said deflection signals indicative of said at rest position and said displaced position, said air bag triggering circuitry being configured for connection to remotely positioned inflation structure having an air bag associated therewith and said air bag triggering circuitry being configured for generating and supplying an inflate signal to said remotely positioned inflation structure for use by said remotely positioned inflation structure to cause inflation of said air bag, and wherein said air bag triggering circuitry is configured to said inflate signal upon receipt of said deflection signal from said determining circuitry.
  • 4. The acceleration change detector of claim 1, wherein said movement inhibitor includes a first magnet connected to said substrate of said second portion and a second magnet fixedly positioned to be moveable when said support moves.
  • 5. The acceleration change detector of claim 1, wherein said deflection sensor is a flexible potentiometer, wherein said substrate is elastically deformable, wherein said electrically conductive material is a conductive ink deposited on said substrate to form an electrical component which has a resistance that varies upon deflection of said substrate.
US Referenced Citations (129)
Number Name Date Kind
3113223 Smith et al. Dec 1963 A
3174125 Curby Mar 1965 A
3229511 Rossire Jan 1966 A
3327270 Garrison Jun 1967 A
3332280 Fish et al. Jul 1967 A
3489917 Gurol Jan 1970 A
3517999 Weaver Jun 1970 A
3541491 Worster Nov 1970 A
3545283 McGunigle Dec 1970 A
3788149 Wilner Jan 1974 A
3820529 Gause et al. Jun 1974 A
3878711 Randolph, Jr. Apr 1975 A
3888117 Lewis Jun 1975 A
3895288 Lampen et al. Jul 1975 A
3958455 Russell May 1976 A
3968467 Lampen et al. Jul 1976 A
3971250 Taylor Jul 1976 A
4023054 Taylor May 1977 A
4038867 Andrews et al. Aug 1977 A
4123158 Reytblatt Oct 1978 A
4152304 Tadewald May 1979 A
4191470 Butter Mar 1980 A
4235141 Eventoff Nov 1980 A
4252391 Sado Feb 1981 A
4258100 Fujitani et al. Mar 1981 A
4258720 Flowers Mar 1981 A
4268815 Eventoff May 1981 A
4269506 Johnson et al. May 1981 A
4273682 Kanamori Jun 1981 A
4276538 Eventoff Jun 1981 A
4301337 Eventoff Nov 1981 A
4306480 Eventoff Dec 1981 A
4314227 Eventoff Feb 1982 A
4314228 Eventoff Feb 1982 A
4315238 Eventoff Feb 1982 A
4355692 Ostrelich Oct 1982 A
4414537 Grimes Nov 1983 A
4420251 James et al. Dec 1983 A
4429580 Testa et al. Feb 1984 A
4444205 Jackson Apr 1984 A
4451714 Eventoff May 1984 A
4461085 Dewar et al. Jul 1984 A
4489302 Eventoff Dec 1984 A
4503705 Polchaninoff Mar 1985 A
4542291 Zimmerman Sep 1985 A
RE32003 Shoberg Oct 1985 E
4575117 Uchida Mar 1986 A
4605593 Iida Aug 1986 A
4639711 Edholm et al. Jan 1987 A
4649784 Fulks et al. Mar 1987 A
4703335 Matsushita et al. Oct 1987 A
4715235 Fukui et al. Dec 1987 A
4729809 Dery et al. Mar 1988 A
4745930 Confer May 1988 A
4748433 Jackson et al. May 1988 A
4763534 Hager Aug 1988 A
4786764 Padula et al. Nov 1988 A
4810992 Eventoff Mar 1989 A
4822040 Raditic Apr 1989 A
4825696 Seipler May 1989 A
4837548 Lodini Jun 1989 A
4876419 Lodini Oct 1989 A
4968965 Naitou et al. Nov 1990 A
4979763 Blackburn Dec 1990 A
5002306 Hiramitsu et al. Mar 1991 A
5059751 Woodman et al. Oct 1991 A
5065322 Mazur et al. Nov 1991 A
5086785 Gentile et al. Feb 1992 A
5109341 Blackburn et al. Apr 1992 A
5134248 Kiec et al. Jul 1992 A
5157372 Langford Oct 1992 A
5172790 Ishikawa et al. Dec 1992 A
5202281 Ishibashi Apr 1993 A
5202831 Blackburn et al. Apr 1993 A
5216607 Diller et al. Jun 1993 A
5222399 Kropp Jun 1993 A
5232243 Blackburn et al. Aug 1993 A
5250227 Margolin Oct 1993 A
5265904 Shelton Nov 1993 A
5265905 Shelton Nov 1993 A
5269559 Filion et al. Dec 1993 A
5269560 O'Loughlin et al. Dec 1993 A
5275432 Pray et al. Jan 1994 A
5297976 VanDerStuyf et al. Mar 1994 A
5308106 Heidorn et al. May 1994 A
5309135 Langford May 1994 A
5313023 Johnson May 1994 A
5344185 Cooke, II Sep 1994 A
5350189 Tsuchitani et al. Sep 1994 A
5364125 Brown et al. Nov 1994 A
5366242 Faigle et al. Nov 1994 A
5369232 Leonelli Nov 1994 A
5371333 Kanai et al. Dec 1994 A
5383473 Moberg Jan 1995 A
5387819 Ueno et al. Feb 1995 A
5388459 Inoue et al. Feb 1995 A
5395802 Kiyota et al. Mar 1995 A
5396439 Yamada Mar 1995 A
5398962 Kropp et al. Mar 1995 A
5399819 Lang et al. Mar 1995 A
5413378 Steffens, Jr. et al. May 1995 A
5419176 Walker May 1995 A
5423227 Polaert et al. Jun 1995 A
5423569 Reighard et al. Jun 1995 A
5439249 Steffens, Jr. et al. Aug 1995 A
5441302 Johnson et al. Aug 1995 A
5443284 Strahl et al. Aug 1995 A
5443286 Cunningham et al. Aug 1995 A
5447327 Jarboe et al. Sep 1995 A
5454589 Bosio et al. Oct 1995 A
5454591 Mazur et al. Oct 1995 A
5456492 Smith et al. Oct 1995 A
5458366 Hock et al. Oct 1995 A
5460405 Faigle et al. Oct 1995 A
5470105 Rose et al. Nov 1995 A
5474328 Nilsson Dec 1995 A
5478111 Marchant et al. Dec 1995 A
5480185 Lowe et al. Jan 1996 A
5483845 Stein et al. Jan 1996 A
5489119 Prescaro et al. Feb 1996 A
5489806 Harris et al. Feb 1996 A
5490411 Hogan Feb 1996 A
5494311 Blackburn et al. Feb 1996 A
5515725 Tabota et al. May 1996 A
5531472 Semchena et al. Jul 1996 A
5583476 Langford Dec 1996 A
5614673 Yamamoto Mar 1997 A
5625333 Clark et al. Apr 1997 A
5665914 Yamamoto Sep 1997 A
Foreign Referenced Citations (2)
Number Date Country
527665 Sep 1976 SU
9113784 Sep 1991 WO