The invention relates to a device for measuring forces applied by a cycling shoe and method for same.
Measurement of the forces applied by a cyclist to a bicycle pedal can be used for a number of purposes. These include calculation of the applied torque and power, detecting whether the cyclist is seated or standing, monitoring the efficiency of the cycling action, and detecting and measuring biomechanical characteristics of the cyclist. Typically, systems that are intended for any of these applications consist of some combination of the following four parts:
The force sensors, motion sensors and processing module are typically located very close to each other, or are integrated with each other, and are connected by short wired links. Typically, the display module is located elsewhere on the bicycle or cyclist and is connected to the processing module via a wired or a wireless link. The processing module takes the values from the force and motion sensors, processes them to produce useful information, and sends the results to the display or recording module.
Pedals used by competitive cyclists are characterised by a locking mechanism whereby a cleat fixed to the underside of the cyclist's shoe engages with the pedal, and maintains the shoe in connection with the pedal under all forces applied by a cyclist during normal operation. The forces of interest while cycling are the forces applied by the cyclist's foot through the sole of the shoe and the cleat into the pedal. During a revolution of the crank, the direction and magnitude of the force exerted by the cyclist on the pedal will vary. The force is most usefully considered as consisting of a pair of orthogonal force vectors. One vector is normal to the plane of the interface between the cleat (which is attached to the sole of the shoe) and the pedal, and one vector is parallel to the plane in the forwards/backwards direction. At any instant, if the magnitudes of the normal and parallel vectors are known then the magnitude and direction of the total force is known.
The normal force vector represents pure compression (push down) or tension (pull up) force on the cleat/pedal interface. The parallel vector represents pure shear (slide forwards or backwards) force on the cleat/pedal interface. Compression force is usually the principal component used by a cyclist to exert force on a pedal, but tension and/or shear force components can form a significant part of the total force exerted by the cyclist at certain points during the revolution of the crank. An accurate force measurement system must include a means to measure compression, tension and shear components of the forces applied by the cyclist to the pedal.
Existing systems for measuring forces applied to a pedal can be divided into two categories. The first category is systems that use force sensors in or on the pedal. These suffer from the limitation that they are not easily moved between bicycles. The measurement sensors are integrated into the pedal, and therefore moving the system to another bicycle requires removal and refitting of the pedals. Examples include U.S. Pat. No. 8,011,242 (O'Neill et al.), PCT Publication No. WO 2012/038677 (Gros et al.), US Patent Publication No. 2011/0067503 (Roudergues et al.), and PCT Publication No. WO 2010/088888 (Biermann et al.).
The second category is systems that use force sensors in or attached to the cyclist's shoe. However, all of the prior art systems of this category are either mounted outside the shoe exposed to the environment, or are limited in their measurement of the total force exerted on the pedal by the cyclist. Systems of this category include:
There are also a number of prior art systems that describe sensors in running or walking shoes. These are generally concerned with measurement of movement, and distribution of pressure on the sole. Systems of this type include:
None of these systems support measurement of tension or shear forces, and therefore they are not usable for accurate measurement of forces in cycling shoes.
It is an object of the present invention to overcome at least one of the above-mentioned problems.
According to the present invention there is provided, as set out in the appended claims, a device for determining power output comprising at least two sensors and a shoe comprising the device.
The present invention overcomes the limitations of the prior art shoe sensors by providing a force measurement device inside the cycling shoe that can measure or calculate compression (push down), tension (pull up) and shear forces that act at the plane of the interface between the cleat and the pedal.
The present invention consists of two parts: a measurement device and a processing method. The first part is a force measurement device inside a cycling shoe, located between the sole of the shoe and the cyclist's foot. The device is a sensor platform that measures compression and tension forces applied by the cyclist through the sole of the shoe to the cleat that is attached to the shoe, and thereby to the pedal of the bicycle. The second part of the invention is a method or algorithm for processing the force sensor outputs to calculate the shear force applied by the cyclist. This allows shear force to be discovered without the need for extra sensors to directly measure it.
In one embodiment the sensor platform is connected to an electronic processing module that is in or attached to the shoe and that executes the algorithm. At regular short intervals (typically many times per second) the processing module takes the outputs from the sensor platform, and applies the algorithm to calculate shear force. There is one sensor platform and one processing module for each shoe. The processing modules on the left and right shoes may communicate with each other by wired or wireless links to exchange values. The processing modules may include measurements from other sensors, and may use all the measurements and calculated values available to them to calculate other quantities such as velocities, angular positions, cadence, pressure, force distribution, torque, and power. The values measured and calculated by the processing modules may be electronically recorded by them for later analysis. The values may also be sent by a wired or a wireless connection to one or more other devices for display or recording or onward transmission to another system.
In one embodiment the sensor platform is located inside the shoe, in a space provided in the sole, so that the sensor platform is directly underneath the area of the cyclist's foot that is used to exert force on the cleat and the pedal. A cleat is typically attached to a cycling shoe using bolts that are screwed into holes in the sole of the shoe. The sensor platform is positioned and/or dimensioned so that it covers the area of the sole that is used to support the cleat, and includes the holes that are used to attach the cleat. The bolts used to fix the cleat pass through the sole of the shoe and are screwed directly into threaded holes in the sensor platform.
In one embodiment the sensor platform includes at least two types of force sensors. The first type is a set of sensors designed to detect compression between the top plate and the bottom plate, and the second type is a set of sensors designed to detect tension from the cleat attachment bolts.
In one embodiment a number of compression sensors are fitted to the sensor platform such that all compressive forces must pass through at least one of the sensors in order to act on the cleat and pedal. A higher number of sensors allow more detailed measurement of the distribution of force applied by the cyclist, and a lower number reduces the cost of manufacture of the sensor platform. The compression sensors may be of any suitable type, arranged to detect a compressive load normal to the plane of the sensor platform.
In one embodiment the tension sensors in the sensor platform are arranged to detect tension forces in the cleat attachment bolts when the cyclist pulls up against the cleat and pedal. The cleat attachment bolts are screwed into the sensor platform, through the sole of the shoe, and the tension sensors are positioned at the bolt holes so that any pull on the bolts is measured by the tension sensors. Typically there are 3 or 4 cleat attachment bolts, and each bolt hole must have an associated tension sensor.
This arrangement of force sensors allows the device to intercept and measure all compression and tension forces applied by the cyclist to the cleat and pedal. These measurements are passed from the sensor platform to the processing module via a communication link.
In one embodiment the processing module may be positioned anywhere in or on the shoe, including within the sensor platform or integrated into the structure of the shoe or in a pocket on the inside or outside of the shoe. The processing module may be a permanent part of the shoe or it may be removable and replaceable by the end user. The connection between the sensor platform and the processing module may be wireless or wired. If it is a wired connection then the connecting wires are integrated into the construction of the shoe and have connectors at each end to facilitate electrical attachment of the sensor platform and the processing module. The connectors are also integrated into the construction of the shoe.
In one embodiment the compression and tension sensors measure forces that are normal to the plane of the sensor platform. It is also useful to know the shear force applied by a cyclist while pedalling. Shear force is force applied along the plane of the sensor platform, either forwards or backwards. Shear force may be measured directly by including shear force sensors in the sensor platform, or it may be calculated from the compression and tension force measurements according to the following algorithm. Using the algorithm avoids the requirement to include shear sensors, thereby reducing the cost and complexity of the sensor platform. If shear force sensors are included in the sensor platform then this algorithm may be used to confirm the calibration of all the sensors by calculating the shear force and comparing it to the measured shear force.
The pedal on a bicycle crank is free to rotate easily around a short axle attached to the end of the crank. In order that the pedal does not rotate around its own axle during pedalling it must be the case that the total moment of forces around the pedal axle is zero at all times. This means that the cyclist must apply force so that the moment of forces tending to rotate the pedal one way around its own axle is exactly equal to the moment of forces tending to rotate the pedal the other way. In fact during typical pedalling action the pedal rotates back and forth, but as there is no great force opposing this rotation the moment of force required to rotate the pedals back and forth is very small with respect to the total forces applied, and therefore the force used to rotate the pedals can be neglected for this algorithm.
If the force applied by a cyclist is completely normal to the plane of the cleat and pedal, and does not include any element of shear force, then the sum of the moments about the pedal axle of the forces measured by each of the compression and tension sensors will be zero.
If the cyclist, while pedalling, includes any component of shear force along the plane of the cleat and pedal then this force will not be directly measured by the compression and tension sensors, because they measure only the components of the forces that are normal to the plane. The shear force is applied at some short distance above the pedal axle determined by the total thickness of the pedal, cleat and sole (typically 1 cm to 2 cm), and therefore it will produce a moment about the pedal axle. However, the sum of the moments about the pedal axle must still be zero, and therefore the moment produced by the shear force must be opposed by a change in the total moment produced by the compression and tension forces. This change in the total moment of the normal forces can be detected by examination of the measurements from the compression and tension sensors, and therefore the magnitude of the shear force can be calculated. That is, if the sum of the moments about the pedal axle calculated from the values from the compression and tension sensors is not equal to zero then the deviation from zero must be due to a shear force component.
In one embodiment there is provided a device for determining power output comprising at least one sensor configured to be accommodated between a foot and a sole of a shoe; wherein the sensor is adapted to measure a compression force applied by a user to a pedal of a bicycle.
In one embodiment there is provided a device for determining power output comprising at least one sensor configured to be accommodated between a foot and a sole of a shoe; wherein the sensor is adapted to measure a tension force applied by a user to a pedal of a bicycle.
The invention will be more clearly understood from the following description of an embodiment thereof, given by way of example only, with reference to the accompanying drawings, in which:—
To be useful and accurate the system must measure all the force exerted by the cyclist on each pedal. In exerting force on a pedal a cyclist applies force from their foot to a shoe, from the shoe to a cleat, and from the cleat to a pedal, as illustrated in
The present invention provides a means to measure or calculate the compression, tension and shear forces by using a force sensor platform 9 inside a sole 10 of a (cycling) shoe 5. The sensor platform 9 is in a specially formed space 24 in the inside surface of the sole 10 so that the space is between the cyclist's foot and the sole of the shoe.
The compression sensors 12 are positioned in the sensor platform 9 so that they are the only significant force path between the top plate 16 and the bottom plate 17, and any compression force applied to the top plate 16 will be detected by one or more of the compression sensors 12. The number of compression sensors 12 fitted may vary to provide the required trade off between detail of measurement and cost of manufacture.
The tension sensors 13 measure all force tending to pull the cleat attachment bolts 15 away from their threaded holes 18 in the sensor platform 9. There is at least one tension sensor 13 for each threaded hole 18 in the sensor platform. One possible arrangement of the tension sensor 13 is shown in
The compression sensors 12 and tension sensors 13 shown in
The sensor platform 9 will detect and directly measure all force applied by a foot inside the shoe 5 pressing downwards on a cleat 6 engaged with a pedal 7, and all force applied by pulling upwards against a cleat 6 engaged with a pedal 7. When the cyclist presses down the forces are measured by the set of compression sensors 12, and the set of tension sensors 13 are not affected because there is no change in the tension in the cleat attachment bolts 15. When the cyclist pulls up the forces are measured by the set of tension sensors 13, and the set of compression sensors 12 are not affected because the cyclist's foot tends to lift off the sole of the shoe and therefore off the top plate 16 of the sensor platform 9.
The sensor platform 9 may include other sensors to measure force or motion. It may include electronic circuits for acquiring and processing the values from those sensors, and electronic circuits to communicate the values to a processing module or display. The connection between the sensor platform 9 and the processing module 3 may be wired or wireless. The processing module 3 may be in any appropriate location in or on the shoe 5, including inside the sensor platform 9, in a separate space in the sole 10 of the shoe 5, in a space formed in the material of the shoe 5, or temporarily or permanently attached to the outside of the shoe 5. The processing module 3 may be installed in the shoe 5 during manufacture and assembly of the shoe, or may be installed by the end user after purchasing the shoe 5 and the processing module 3.
In another arrangement, the sensor platform 9 or the processing module 3, or both, are permanently assembled into the shoe 5 during manufacture of the shoe and are permanently attached to the cable 22.
The processing module 3 and the sensor platform 9 may be powered by one or more batteries that may be inside the processing module 3 or the sensor platform 9 or may be separate from them. The batteries may be replaceable by the end user or may be rechargeable by the end user. If they are replaceable then the location of the batteries facilitates access to them by the end user. If they are rechargeable then there is an electrical input socket accessible when the shoe 5 is not in use and not being worn.
The processing module 3 takes the values from various sensors on the shoe 5, including the compression sensors 12 and tension sensors 13 in the sensor platform 9. The module 3 processes the sensor values many times per second to calculate various results, and sends the results by a wired or wireless connection to one or more display and/or recording devices 4.
The present invention includes an algorithm by which the processing module 3 uses the values from the compression and tension force sensors 12,13 to calculate the shear force being applied by the cyclist. The algorithm is based on the principal that the total of the moments of forces around the pedal axle must be zero, or negligibly close to zero, at all times. The moment of a force is calculated as the magnitude of the force multiplied by the perpendicular distance from the line of action of the force to the centre of rotation. Moments tending to rotate the pedal one direction have an opposite sign to moments tending to rotate the pedal the other direction. Any apparent non-zero total moment calculated from the outputs of the compression and tension sensors must be due to compensating force being applied to oppose the moment caused by a shear force.
F
cw
×d
cw
=F
acw
×d
acw
In a general case with a number of compression and tension sensors measuring forces at specific points, each measured force has a clockwise or an anticlockwise moment around the pedal axle 20 and the sum of clockwise moments must equal the sum of anticlockwise moments:
Σ(Fcw×dcw)=Σ(Facw×dacw)
(Fcw×dcw)+(Fs×ds)=Facw×dacw
In the general case, with a number of compression and tension sensors measuring forces at different points in the sensor platform:
Σ(Fcw×dcw)+(Fs×ds)=Σ(Facw×dacw)
All the compression and tension forces Fcw and Facw are measured, the perpendicular distances dcw and dacw from each force sensor to the pedal axle are known, and the distance ds from the sensor platform to the pedal axle is known, therefore the shear force Fs can be calculated:
F
s=(Σ(Facw×dacw)−Σ(Fcw×dcw))/ds
In practice the perpendicular distances from each of the compression and tension sensors 12,13 to the pedal axle 20 will depend on the exact position of the cleat 6 on the sole 10 of the shoe 5. Typically there is some small positional adjustment possible when the cleat 6 is being bolted to the sole 5 by a user, and this will affect the relationship between the sensors 12, 13 and the pedal axle 20. The positional relationship between the cleat 6 and the pedal 7 is not changed by how the cleat 6 is bolted to the shoe 5; it is the relationship between the shoe 5 and the cleat 6 that is affected. Therefore the relationship between the sensor platform 9 and the pedal 7 is affected, and the perpendicular distances from the force sensors 12, 13 to the pedal axle 20 may change. Therefore the possible variation in these perpendicular distances must be measured in order for this algorithm to be accurate.
There are obviously corresponding changes to the perpendicular distances for all the compression and tension sensors 12, 13 in the sensor platform 9 if the cleat 6 is rotated and/or shifted from the ideal position. These distances from each sensor 12,13 to the pedal axle position 19 are required for the algorithm that calculates shear force, and therefore it is necessary to know the exact position of the cleat 6 on the sole 10 of the shoe 5 after the user has bolted it on.
The position of the cleat 6 on the sole 10 can be determined by observing it after it has been bolted on.
The algorithm also calculates the balance of the forces across the width of the pedal 7 at each sample time. This provides a measure of how evenly the cyclist distributes force across the pedal 7 and how that varies as they cycle. Standard mathematical formulae can be used to calculate the effective centre of the total applied force, from the forces measured by the compression and tension sensors 12,13 in the sensor platform. The location of this centre of force along the width of the sensor platform 9 indicates whether the cyclist is applying force towards one side of the pedal 7 or the other, or equally on both sides.
The use of the algorithm is not limited to use with values from the measurement device described here. The algorithm can be used to calculate shear force for any system that measures compression and tension forces in the plane of the cleat/pedal interface. That includes systems that place force sensors between the sole 5 and the cleat 6, inside the cleat 6, between the cleat 6 and the pedal 7, and inside the pedal 7. All that is necessary for the algorithm is measurement values from a set of compression and force sensors distributed on both sides of the pedal axle, the perpendicular distances from each sensor to the pedal axle, and the perpendicular distance dS from the sole of the shoe to the pedal axle. The shear force is assumed to be applied by the cyclist's foot such that it acts along the sole of the shoe parallel to the cleat/pedal interface, and therefore dS is the distance that gives the shear force a rotational moment about the pedal axle.
In the specification the terms “comprise, comprises, comprised and comprising” or any variation thereof and the terms “include, includes, included and including” or any variation thereof are considered to be totally interchangeable and they should all be afforded the widest possible interpretation and vice versa.
The embodiments in the invention described with reference to the drawings comprise a computer apparatus and/or processes performed in a computer apparatus. However, the invention also extends to computer programs, particularly computer programs stored on or in a carrier adapted to bring the invention into practice. The program may be in the form of source code, object code, or a code intermediate source and object code, such as in partially compiled form or in any other form suitable for use in the implementation of the method according to the invention. The carrier may comprise a storage medium such as ROM, e.g. CD ROM, or magnetic recording medium, e.g. a floppy disk or hard disk. The carrier may be an electrical or optical signal which may be transmitted via an electrical or an optical cable or by radio or other means.
The invention is not limited to the embodiments hereinbefore described but may be varied in both construction and detail.
Number | Date | Country | Kind |
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1212299.0 | Jul 2012 | GB | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2013/064744 | 7/11/2013 | WO | 00 |