The disclosed embodiments relate generally to calibrating sensors used for determination of a navigational state of a human interface device.
A human interface device (e.g., a mouse, a trackball, etc.) may be used to interact with objects within a user interface. Some applications may need to know the navigational state (e.g., attitude and/or position) of the human interface device while the device is moving. One such example is an application that interfaces with a human interface device that may be moved freely in space (e.g., in one, two, or three dimensions of displacement and one, two or three dimensions of rotation or attitude) to position a cursor in a user interface, adjust display of overlaid objects in an augmented reality application or select a portion of a virtual world for display to a user of the device. However, sensors such as magnetometers and accelerometers that are used to determine the navigational state of a human interface device frequently have non-ideal characteristics coming straight from the factory and additional non-ideal characteristics may be introduced when integrating the sensors into the human interface device. These non-ideal characteristics may cause the device to function poorly or malfunction entirely.
While, compensating for these non-ideal characteristics by calibrating the sensors can substantially improve the performance of the device, conventional calibration techniques require additional steps during manufacturing where the device is positioned in precisely defined navigational states. These additional steps add to the complexity and cost of manufacturing the device. Accordingly, it would be highly desirable to provide a way to calibrate sensors in a human interface device in an effective and cost efficient manner.
Some embodiments provide a method for, at a device including a magnetometer and an accelerometer: calibrating the magnetometer, and for each of a plurality of sample orientations: generating a set of one or more calibrated magnetometer measurements via the magnetometer, and generating a set of one or more uncalibrated accelerometer measurements. The method further includes calibrating the accelerometer using respective calibrated magnetometer measurements and corresponding respective uncalibrated accelerometer measurements for one or more respective sample orientations of the plurality of sample orientations.
In some embodiments, calibrating the magnetometer comprises using a sphere fit technique to calibrate the magnetometer. In some embodiments, calibrating the magnetometer comprises performing magnetometer calibration operations after the magnetometer has been integrated into circuitry of the device. In some embodiments, calibrating the magnetometer comprises storing conversion values for converting uncalibrated magnetometer measurements to calibrated magnetometer measurements and generating a calibrated magnetometer measurement for a respective sample orientation comprises receiving a respective uncalibrated magnetometer measurement from the magnetometer while the device is in a respective sample orientation and converting the respective uncalibrated magnetometer measurement to a respective calibrated magnetometer measurement using the conversation values.
In some embodiments, calibrating the accelerometer comprises comparing a first estimated acceleration with a second estimated acceleration, the first estimated acceleration is determined based on actual accelerometer measurements from the accelerometer and the second estimated acceleration is determined based on an attitude of the device determined using a tri-axial attitude determination. In some embodiments, calibrating the accelerometer comprises using respective calibrated magnetometer measurements and uncalibrated accelerometer measurements for three or more sample orientations. In some embodiments, the device is positioned in a series of sample orientations with at least a minimum spatial diversity and, optionally, the device is positioned in each sample orientation for at least a predefined threshold amount of time.
Some embodiments provide a method for, at a device including a first accelerometer and a second accelerometer: calibrating the first accelerometer and calibrating the second accelerometer. The method further includes calibrating a combined-sensor output to generate combined-sensor conversion values for converting uncalibrated combined-sensor measurements of the combined-sensor output to calibrated combined-sensor measurements of the combined-sensor output. The combined-sensor output includes contributions from the first accelerometer and the second accelerometer. The method also includes adjusting the calibration of the first accelerometer in accordance with the combined-sensor conversion values. In some embodiments, the combined-sensor output is based on a difference between measurements of the first accelerometer and measurements of the second accelerometer.
In some embodiments, calibrating the first accelerometer includes storing first-accelerometer conversion values for converting uncalibrated accelerometer measurements of the first accelerometer to calibrated accelerometer measurements of the first accelerometer. In some embodiments, calibrating the second accelerometer includes storing second-accelerometer conversion values for converting uncalibrated accelerometer measurements of the second accelerometer to calibrated accelerometer measurements of the second accelerometer. In some embodiments, calibrating the first accelerometer includes calibrating scale and/or offset of the first accelerometer and adjusting the calibration of the first accelerometer includes adjusting the calibration of skew and/or rotation of the first accelerometer.
In some embodiments, the method further includes adjusting the calibration of the second accelerometer in accordance with the calibrated combined-sensor output. In some embodiments, calibrating the second accelerometer includes calibrating scale and/or offset of the second accelerometer and adjusting the calibration of the second accelerometer includes adjusting the calibration of skew and/or rotation of the second accelerometer. In some embodiments, adjusting the calibration of the first accelerometer includes adjusting a respective first-accelerometer conversion value in accordance with a particular combined-sensor conversion value and adjusting the calibration of the second accelerometer includes adjusting a respective second-accelerometer conversion value that corresponds to the respective first-accelerometer conversation value in accordance with the particular combined-sensor conversion value. In some embodiments, the operations of calibrating the first accelerometer, calibrating the second accelerometer and calibrating the combined sensor output are performed using sensor measurements from a same plurality of sample orientations.
In accordance with some embodiments, a computer system (e.g., a human interface device or a host computer system) includes one or more processors, memory, and one or more programs; the one or more programs are stored in the memory and configured to be executed by the one or more processors and the one or more programs include instructions for performing the operations of any of the methods described above. In accordance with some embodiments, a non-transitory computer readable storage medium (e.g., for use by a human interface device or a host computer system) has stored therein instructions which when executed by one or more processors, cause a computer system (e.g., a human interface device or a host computer system) to perform the operations of any of the methods described above.
Like reference numerals refer to corresponding parts throughout the drawings.
Human interface devices that have a determinable multi-dimensional navigational state (e.g., one or more dimensions of displacement and/or one or more dimensions of rotation or attitude) are becoming increasingly common for providing user input for many different types of user interfaces. For example, such a human interface device may be used as a multi-dimensional pointer to control a pointer (e.g., a cursor) on a display of a personal computer, television, gaming system, etc. As another example, such a human interface device may be used to provide augmented reality views (e.g., by overlaying computer generated elements over a display of a view of the real world) that change in accordance with the navigational state of the human interface device so as to match up with a view of the real world that is detected on a camera attached to the human interface device. As yet another example, such a human interface device may be used to provide views of a virtual world (e.g., views of portions of a video game, computer generated simulation, etc.) that change in accordance with the navigational state of the human interface device so as to match up with a virtual viewpoint of the user based on the orientation of the device. In this document, the terms orientation, attitude and rotation are used interchangeably to refer to the orientation of a device or object with respect to a frame of reference.
In order to function properly (e.g., return results to the user that correspond to movements of the human interface device in predictable ways), these applications rely on well calibrated sensors that provide a consistent and accurate mapping between the sensor outputs and the navigational state of the human interface device. While specific use cases are described above and will be used to illustrate the general concepts described below, it should be understood that these examples are non-limiting examples and that the embodiments described herein would apply in an analogous manner to any human interface device that would benefit from calibrated sensors.
Attention is now directed to
Thus, the user can use Device 102 to issue commands for modifying the user interface, control objects in the user interface, and/or position objects in the user interface by moving Device 102 so as to change its navigational state. In some embodiments, Device 102 is sensitive to six degrees of freedom: displacement along the x-axis, displacement along the y-axis, displacement along the z-axis, yaw, pitch, and roll.
In some embodiments, the wireless interface is selected from the group consisting of: a Wi-Fi interface, a Bluetooth interface, an infrared interface, an audio interface, a visible light interface, a radio frequency (RF) interface, and any combination of the aforementioned wireless interfaces. In some embodiments, the wireless interface is a unidirectional wireless interface from Device 102 to Host 101. In some embodiments, the wireless interface is a bidirectional wireless interface. In some embodiments, bidirectional communication is used to perform handshaking and pairing operations. In some embodiments, a wired interface is used instead of or in addition to a wireless interface. As with the wireless interface, the wired interface may be a unidirectional or bidirectional wired interface.
In some embodiments, data corresponding to a navigational state of Device 102 (e.g., raw measurements, calculated attitude, correction factors, position information, etc.) is transmitted from Device 102 and received and processed on Host 101 (e.g., by a host side device driver). Host 101 uses this data to generate current user interface data (e.g., specifying a position of a cursor and/or other objects in a user interface).
Attention is now directed to
In some embodiments, the one or more processors (e.g., 1102,
Attention is now directed to
As one example, in
One goal of sensor calibration is to improve the accuracy of sensor measurements from the uncalibrated sensors, which produce “raw” sensor measurements. In some embodiments, calibration is accomplished by determining a set of conversion values that can be used to compensate for error in raw sensor measurements. The error can be modeled as an affine transformation (linear matrix transformation plus offset term), and the goal of calibration is to compute the inverse of the modeled affine transformation; the inverse of the modeled affine transformation is sometimes called a calibration transformation, which is another affine transformation. This calibration transformation includes matrix D (Equation 1) which accounts for error in skew, scale and rotation distortions and an offset ({right arrow over (b)}). In Equation 1, the raw sensor output (“{right arrow over (y)}raw”) is the distorted measurement data that the sensor actually measures, and the calibrated sensor output (“{right arrow over (y)}calibrated”) comes from the application of the calibration transformation to the raw sensor output. This calibrated sensor output is then available for use by other algorithms. In some embodiments, navigational state determination algorithms determine the navigational state of the device based on the calibrated sensor output. For a three dimensional sensor, D is a 3×3 matrix and {right arrow over (b)} is a 3 component vector. For a two dimensional sensor, D is a 2×2 matrix and {right arrow over (b)} is a 2 component vector. For a single dimensional sensor, D and {right arrow over (b)} are both scalar values.
{right arrow over (y)}calibrated=(I+D){right arrow over (y)}raw+{right arrow over (b)} (1)
In some circumstances it is beneficial to separate the rotation from the skew and scale components of the conversion values. For example, the D matrix can be decomposed via polar decomposition to a symmetric matrix (I+S) where I is the identity matrix, S is a matrix that defines scale and skew conversion values and R is an orthonormal rotation matrix, as shown in Equations 2 and 3 below.
In all, in this example, there are twelve conversion values to estimate for each sensor, three offset values, three scale values, three skew values, and three rotation values (as Euler angles). Thus, R is a function of three values (rotation values) and S is a function of six values (three scale values and three skew values).
Many devices use MEMS (Microelectromechanical system) sensors due to the attractive price/performance characteristics of MEMS sensors. In particular MEMS sensors are typically relatively inexpensive and, when properly calibrated, provide sensor measurements that are sufficiently accurate for most commercial applications in consumer electronic devices such as cell phones, cameras and game controllers. Calibration of a MEMS sensor typically required collecting sensor measurements having sufficient measurement diversity in the measurement space for the MEMS sensor. For example, for an accelerometer or a magnetometer the measurement space is orientation based and thus measurement diversity for an accelerometer or magnetometer means collecting sensor values from the accelerometer or magnetometer to a plurality of different device orientations. In contrast, for a gyroscope, the measurement space is movement based, and thus measurement diversity for a gyroscope means collecting sensor values from the gyroscope while Device 102 is rotating about different axes.
While many different combinations of sensors can be used to determine a navigational state of a device, one combination that provides measurements of navigational state that are sufficiently accurate and low cost for many commercial applications is a set of sensors including at least one multi-dimensional magnetometer and one or more multi-dimensional accelerometers. As described above, incorporation of these sensors into a device may introduce error (e.g., “non-ideal” sensor characteristics) and thus recalibration of the sensors after device assembly may be beneficial for improving the accuracy of the sensors. However, calibrating these sensors separately may fail to produce sufficiently accurate calibrations. In particular, accelerometers can be calibrated more effectively by using additional sensor inputs (e.g., magnetometer measurements) as additional inputs to the calibration process, as illustrated in
In some embodiments it is advantageous to calibrate 402 a Magnetometer (e.g., 220-2 in
Attention is now directed to
The following operations are all performed after Device 102 has been assembled (502). Even in circumstances where the sensors are calibrated prior to incorporation into Device 102, additional error may be introduced in the process of assembling Device 102 so that the accuracy of the sensors will be improved by calibrating the sensors once Device 102 has been assembled. For example, the sensors may not be well aligned with the housing of Device 102 and/or the steps required to incorporate the sensors into Device 102 (e.g., soldering, etc.) may introduce sensor error by placing mechanical or thermal stress on the sensor.
Prior to calibrating the one or more accelerometers, Device 102 collects (504) uncalibrated magnetometer measurements and determines if there is a sufficient diversity of magnetometer measurements. In accordance with a determination by Device 102 that there is not (506) a sufficient diversity of magnetometer measurements, Device 102 continues to collect uncalibrated magnetometer measurements. However, in accordance with a determination by Device 102 that there is (508) a sufficient diversity of magnetometer measurements, Device 102 uses the collected uncalibrated magnetometer measurements to calibrate (510) the magnetometer.
Once the magnetometer has been calibrated, Device 102 moves on to calibrating the accelerometer. Device 102 collects (512) calibrated magnetometer measurements and uncalibrated accelerometer measurements and determines if there is a sufficient diversity of accelerometer measurements. In some embodiments, for each sample attitude of Device 102, the uncalibrated accelerometer measurement is associated with the calibrated magnetometer measurement, so that the calibrated magnetometer measurement can be retrieved and used to assist in calibration of the accelerometer in conjunction with the associated uncalibrated accelerometer measurement. In some embodiments, retrieving a calibrated magnetometer measurement includes retrieving an uncalibrated magnetometer measurement and adjusting the uncalibrated magnetometer measurement with magnetometer conversion values to produce a calibrated magnetometer measurement. In some embodiments, the calibrated magnetometer measurement is stored, while in other embodiments, the uncalibrated magnetometer measurement and magnetometer conversion values are stored and the uncalibrated magnetometer measurement is retrieved and adjusted with the magnetometer conversion values in response to requests for the calibrated magnetometer measurement.
In accordance with a determination by Device 102 that there is not (514) a sufficient diversity of accelerometer measurements, Device 102 continues to collect calibrated magnetometer measurements and uncalibrated accelerometer measurements. However, in accordance with a determination by Device 102 that there is (516) a sufficient diversity of accelerometer measurements, Device 102 uses the collected calibrated magnetometer measurements and uncalibrated accelerometer measurements to calibrate (518) the accelerometer(s), as described in greater detail below with reference to
Once the magnetometer and one or more accelerometers have been calibrated, the sensors can be used to determine (522) a navigational state (e.g., orientation and/or position) of Device 102 (e.g., using a Kalman filter as described in greater detail in U.S. Pat. Pub. No. 2010/0174506).
It should be understood that the particular order in which the operations in
Attention is now directed to
Device 102 (e.g., the human interface device including a magnetometer and an accelerometer) calibrates (602) the magnetometer. In some embodiments, calibrating the magnetometer comprises using (604) a sphere fit technique to calibrate the magnetometer, as described in greater detail below with reference to Equation 4. In some embodiments, calibrating the magnetometer comprises performing (606) magnetometer calibration operations after the magnetometer has been integrated into circuitry of Device 102, so that the calibration takes into account any non-ideal characteristics introduced during the process of incorporating the magnetometer into Device 102. In some embodiments, calibrating the magnetometer comprises storing (608) magnetometer conversion values for converting uncalibrated magnetometer measurements to calibrated magnetometer measurements.
The magnetic calibration is based on the sphere fit model, whereby the estimated states are used to remove linear distortions. The uncalibrated measurements from a magnetometer will typically initially resemble a non-spherical ellipsoid. The goal is to fit the distorted measurements into a uniform sphere by adjusting the magnetometer conversion values x1-x9 by reducing error (“e” in Equation 4) for a diverse set of magnetometer measurements. In some embodiments, collecting a diverse set of magnetometer measurement includes, for each new magnetometer measurement determining if the new magnetometer measurement is sufficiently different, by Euclidean distance in the measurement space, from all the previously gathered ones. If the new magnetometer measurement is sufficiently different from previously gathered magnetometer measurements, then the new magnetometer measurement is stored for use in calibrating the magnetometer. If the new magnetometer measurement is not sufficiently different from previously gathered magnetometer measurements, then the new magnetometer measurement is ignored and/or discarded.
Equation 4 provides one example of an equation that can be used to determine a set of magnetometer conversion values x1-x9 for a magnetometer using a sphere fit.
In Equation 4, magnetometer conversion values x1-x3 correspond to offset, magnetometer conversion values x4-x6 correspond to scale, and magnetometer conversion values x7-x9 correspond to skew and, optionally, rotation. In this example, an estimation of the error (e) calculated in accordance with Equation 4 and subsequently used to determine updated magnetometer conversion values, which are, in turn, used to generate a subsequent error estimations using the Gauss-Newton method.
For a first iteration, the magnetometer conversion values (x) in Equation 4 are set to a predefined value (e.g., zero or some other starting value), and for each magnetometer measurement in the diverse set of magnetometer measurements, a value for (e) is calculated. For each of a plurality of sequential iterations, adjustments to the magnetometer conversion values (x) are determined based on the estimated error (e), using the well-known Gauss-Newton method. A more complete description of implementing the Gauss-Newton method is provided in “Derivative free analogues of the Levenberg-Marquardt and Gauss algorithms for nonlinear least squares approximation”, Kenneth M. Brown and J. E. Dennis, 1970. Numer. Math. 18, 287-297 (1972), which is incorporated herein by reference in its entirety. The adjusted magnetometer conversion values determined in the current iteration are used to generate values of the estimated error (e) for the next iteration. Iterations are repeated until the magnetometer conversion values produce an estimated error (e) that is sufficiently small (e.g., below a predefined threshold). Typically, magnetometer conversion values that produce an acceptably small error can be produced with approximately 20-30 iterations. Performing additional iterations of the Gauss-Newton method will generally not increase the accuracy of the magnetometer after convergence has been reached (i.e., the error value (e) has reached a minimum). However, in some implementations fewer than 20-30 iterations of the Gauss-Newton method can be used if computational resources are scarce, as additional iterations increase the time and computational resources (memory, processing power, etc.) that are consumed by the calibration process. Thus, the number of iterations can be adjusted in accordance with the desired tradeoff between accuracy and speed/computational resources. It should be understood that while the Gauss-Newton estimation method is described as one possible approach for performing a sphere fit, many other options exist, for example a Kalman filter could be used to iteratively estimate the magnetometer conversion values as each magnetometer measurement is received.
In some embodiments, after calibrating the magnetometer, one or more accelerometers are calibrated (610) using the calibrated magnetometer. In some embodiments, Device 102 is positioned (612) in a series of sample orientations with at least a minimum spatial diversity. It should be understood that the series of sample orientations could be a set of predefined sample orientations or a set of opportunistically captured sample orientations. When the sample orientations are opportunistically captured, typically more sample orientations are needed to achieve the minimum spatial diversity. Typically, the order in which the sample orientations are captured is not critical. However in some implementations, a user may be instructed to place Device 102 in a sequence of predefined approximate orientations so as to ensure that the minimum spatial diversity of measurements is reached quickly. In some embodiments, collecting a diverse set of accelerometer measurement includes, for each new accelerometer measurement determining if the new accelerometer measurement is sufficiently different, by Euclidean distance in the measurement space, from all the previously gathered ones. If the new accelerometer measurement is sufficiently different from previously gathered accelerometer measurements, then the new accelerometer measurement is stored for use in calibrating the accelerometer. If the new accelerometer measurement is not sufficiently different from previously gathered accelerometer measurements, then the new accelerometer measurement is ignored and/or discarded. In some embodiments the determination as to whether or not a set of sensor measurements has sufficient spatial diversity is based at least in part on the quality of measurements in the set of sensor measurements. In other words, the lower the noise of the sensor measurements, the less spatially diverse the sensor measurement need to be to be determined to have sufficient spatial diversity. In some embodiments, an angular separation of at least 30 degrees between sensor measurements yields “sufficient” spatial diversity of measurements.
In some embodiments, Device 102 is positioned (614) in each sample orientation for at least a predefined threshold amount of time (e.g., 1 second, 3 seconds or any reasonable amount of time) in order to allow Device 102 to acquire an accelerometer measurement without an acceleration component due to the movement of Device 102 from a previous orientation.
Operations 618-630 are performed (616) for each of a plurality of sample orientations. Device 102 generates (618) a set of one or more calibrated magnetometer measurements via the magnetometer. In some embodiments, generating a calibrated magnetometer measurement for a respective sample orientation comprises receiving (620) a respective uncalibrated magnetometer measurement from the magnetometer while Device 102 is in a respective sample orientation and converting (622) the respective uncalibrated magnetometer measurement to a respective calibrated magnetometer measurement using the conversation values.
Device 102 generates (624) a set of one or more uncalibrated accelerometer measurements. Device 102 calibrates (626) the accelerometer using respective calibrated magnetometer measurements and corresponding respective uncalibrated accelerometer measurements for one or more respective sample orientations of the plurality of sample orientations (e.g., as described in greater detail below with reference to Equations 5-6). In some embodiments, calibrating the accelerometer comprises (628) comparing a first estimated acceleration with a second estimated acceleration, where the first estimated acceleration is determined based on actual accelerometer measurements from the accelerometer and the second estimated acceleration is determined based on an attitude of Device 102 determined using a tri-axial attitude determination (e.g., CTRIAD in Equation 6 below). In some embodiments, calibrating the accelerometer comprises using (630) respective calibrated magnetometer measurements and uncalibrated accelerometer measurements for three or more sample orientations.
Equations 5-6 provides one example of equations that can be used to determine a set of accelerometer conversion values x1-x7 for an accelerometer using a calibrated magnetometer.
In Equations 5-6, accelerometer conversion values x1-x3 correspond to offset, accelerometer conversion values x4-x6 correspond to scale and accelerometer conversion value x7 corresponds to an estimation of the angle between the local magnetic field and gravity (e.g., a value based on the local magnetic inclination, which is an angle between the Earth's magnetic field and the Earth's surface proximate to Device 102). The off-diagonal terms in the D matrix, which would account for skew and rotation are ignored in the particular embodiment described above, but could be calculated in an alternative embodiment. In some embodiments, the off-diagonal terms are calculated using the method described below with reference to Equations 7-12. In this example, an estimation of the corrected acceleration is calculated in accordance with Equation 5 using the estimated accelerometer conversion values and the results are compared with an alternative estimation of acceleration that is based on a measurement from the calibrated magnetometer (and thus will typically be more accurate, as the magnetometer has already been calibrated) to determine an estimated accelerometer error ({right arrow over (e)}).
In particular, in Equation 6, the estimated acceleration using the sensor model from Equations 1 and 5 is compared with an estimated acceleration due to gravity that should be detected by the sensor in the orientation at which the sensor measurements were determined. In order to determine this estimated acceleration due to gravity, the orientation of the sensor is estimated using a “Tri-Axial Attitude Determination” (hereinafter TRIAD) method that takes measured acceleration, measured magnetic field, a reference magnetic field and a reference acceleration into account to determine an orientation, as described in greater detail in H. D. Black, “A Passive System for Determining the Attitude of a Satellite,” AIAA Journal, Vol. 2, July 1964, pp. 1350-1351. With the assumption that Device 102 is located near the Earth's surface, the average acceleration at the Earth's surface (e.g., [0,0,9.8] m/s2) can be used as the reference acceleration, and the reference magnetic field can be determined using the reference acceleration (gravity) and an estimated angle between gravity and the Earth's magnetic field. Thus, CTRIAD in Equation 6 takes as inputs: the calibrated measured acceleration (using coefficients determined in a prior iteration), the calibrated measured magnetic field (using the calibrated magnetometer), an estimated angle between gravity and the Earth's magnetic field. The orientation determined by CTRIAD is multiplied by the average acceleration at the Earth's surface (e.g., [0,0,9.8] m/s2) to get a different estimate of acceleration of Device 102. The comparison of the accelerometer-only estimation of acceleration from Equation 5 with the combined accelerometer/magnetometer estimation of acceleration, which is typically more accurate because it uses an additional measurement (e.g., a calibrated magnetometer measurement) from a calibrated sensor, enables the accelerometer conversion values for the accelerometer-only estimation of acceleration to be adjusted more to improve the precision of the accelerometer-only estimation of acceleration using the Gauss-Newton method, as described in greater detail below.
For a first iteration, the accelerometer conversion values (x) in Equations 5-6 are set to a predefined value (e.g., zero or some other starting value), and for each accelerometer measurement in the diverse set of accelerometer measurements, a corrected accelerometer measurement is determined (e.g., using Equation 5). Subsequently, an estimated accelerometer error ({right arrow over (e)}) is determined by comparing the corrected accelerometer measurement with an estimated acceleration determined based on an estimated orientation determined using the corrected accelerometer measurement and a corresponding magnetometer measurement (e.g., using Equation 6). For each of a plurality of sequential iterations, adjustments to the accelerometer conversion values (x) are determined based on the value of the estimated accelerometer error ({right arrow over (e)}) using the Gauss-Newton method (e.g., adjusting the accelerometer conversion values in a way that will reduce the estimated accelerometer error ({right arrow over (e)}). The adjusted accelerometer conversion values determined in the current iteration are used to generate values for estimated accelerometer error ({right arrow over (e)}) for the next iteration.
In some embodiments, when multiple accelerometer measurements acquired at different device orientations are used to calibrate the accelerometer, during a single iteration a different estimated accelerometer error ({right arrow over (e)}) is calculated for each accelerometer measurement of the multiple accelerometer measurements using the same set of accelerometer conversion values (x), and the adjustments to the accelerometer conversion values are determined for all of the accelerometer measurements in the multiple accelerometer measurements. In other words, each iteration includes determining an estimated accelerometer error ({right arrow over (e)}) for each accelerometer measurement and adjusting the shared accelerometer conversion values (x) so as to minimize these estimated accelerometer errors, on average. Iterations are repeated until the accelerometer conversion values produce an estimated accelerometer error that is sufficiently small (e.g., below a predefined threshold). Typically, accelerometer conversion values that produce an acceptably small error can be generated with approximately 20-30 iterations. Performing additional iterations of the Gauss-Newton method will generally not increase the accuracy of the accelerometer after convergence has been reached (i.e., the error value (e) has reached a minimum). However, in some implementations fewer than 20-30 iterations of the Gauss-Newton method can be used if computational resources are scarce, as additional iterations increase the time and computational resources (memory, processing power, etc.) that are consumed by the calibration process. Thus, the number of iterations can be adjusted in accordance with the desired tradeoff between accuracy and speed/computational resources. It should be understood that while the Gauss-Newton estimation method is described as one possible approach for calibrating an accelerometer based on a TRIAD estimation of attitude, many other options exist, for example a Kalman filter could be used to iteratively estimate the accelerometer conversion values as each set of accelerometer and magnetometer measurements is received.
It should be understood that the particular order in which the operations in
Attention is now directed to
Device 102 (e.g., the human interface device that includes multiple accelerometers) calibrates (702) a first accelerometer. In some embodiments, calibrating the first accelerometer includes storing (704) first-accelerometer conversion values (e.g., values (x) for a skew/scale matrix D1 and a displacement vector b1) for converting uncalibrated accelerometer measurements of the first accelerometer to calibrated accelerometer measurements of the first accelerometer. Device 102 calibrates (706) the second accelerometer. In some embodiments, calibrating the second accelerometer includes storing (708) second-accelerometer conversion values (e.g., values (x) for a skew/scale matrix D2 and a displacement vector {right arrow over (b)}2) for converting uncalibrated accelerometer measurements of the second accelerometer to calibrated accelerometer measurements of the second accelerometer. In one implementation, the first and second accelerometers are each separately calibrated using the calibration described above with reference to Equation 4 above.
Device 102 also calibrates (710) a combined-sensor output to generate combined-sensor conversion values (e.g., differential conversion values) for converting uncalibrated combined-sensor measurements of the combined-sensor output to calibrated combined-sensor measurements of the combined-sensor output, where the combined-sensor output includes contributions from the first accelerometer and the second accelerometer. In some embodiments, the combined-sensor output is (712) based on a difference between measurements of the first accelerometer and measurements of the second accelerometer, as described below with reference to Equations 7-9. In some embodiments, the operations of calibrating the first accelerometer, calibrating the second accelerometer and calibrating the combined sensor output are performed using (714) sensor measurements from a same plurality of sample orientations.
For example, in Equations 7-9, below, the combined-sensor output ({right arrow over (a)}diff) is the difference between the output of a first accelerometer and the output of a second accelerometer. In this example, the error is a difference between the corrected accelerometer measurement ({right arrow over (a)}diff) and an alternative estimation of acceleration that is based on an estimated orientation of Device 102 in accordance with the TRIAD method, described above. In some embodiments, the CTRIAD orientation is determined using {right arrow over (a)}diff, and the error estimation and proceeds as described above with reference to Equation 6. However, in other embodiments, the CTRIAD orientation is simply a previously calculated orientation generated using output from one of the accelerometers. In some implementations the accelerometer that is chosen is the accelerometer that will typically be closest to the user's hand when Device 102 is in operation (e.g., the accelerometer closest to a handhold of Device 102, such as accelerometer 220-3 in
Determining an estimated error of the combined-sensor output ({right arrow over (a)}diff) enables estimation of the difference between accelerometer conversion values for the two accelerometers (represented below as (D2−D1) and (b2−b1)). It should be understood, that these combined-sensor conversion values are not calculated using previously calculated accelerometer conversion values for the individual accelerometers, rather, new combined-sensor conversion values Dd and {right arrow over (b)}d are calculated and these combined-sensor conversion values represent differences between the accelerometer conversion values of the two accelerometers. These combined-sensor conversion values are particularly advantageous for determining accelerometer conversion values for skew and rotation terms. In particular, in Equations 7-9, the off-diagonal (skew and rotation) terms' contributions to the error are the same order of magnitude as compared to the diagonals.
In Equations 7-12, combined-sensor conversion values x1-x3 correspond to offset, combined-sensor conversion values x4-x6 correspond to scale and combined-sensor conversion values x7-x12 correspond to skew and, optionally, rotation. In this example, an estimated differential accelerometer error ({right arrow over (e)}) (e.g., calculated in accordance with Equation 7) is calculated and used to determine updated combined-sensor conversion values, which are, in turn, used to generate a subsequent error estimations using the Gauss-Newton method. In this example, an estimation of the differential acceleration ({right arrow over (a)}diff) is calculated in accordance with measurements from the two accelerometers and an alternative estimation of differential acceleration is calculated in accordance with the attitude of Device 102 (e.g., determined in accordance with calibrated magnetometer measurements, calibrated accelerometer measurements from one of the accelerometers and an estimated angle between gravity and the Earth's magnetic field using the TRIAD method). The combined-sensor conversion values (x) in Equations 8-9 are determined using the Gauss-Newton method.
For a first iteration, the combined-sensor conversion values (x) in Equations 8-9 are set to a predefined value (e.g., zero or some other starting value), and for each accelerometer measurement in the diverse set of accelerometer measurements, a corrected accelerometer measurement is determined (e.g., using Equation 5 with the previously identified accelerometer conversion values for the accelerometer). Subsequently, an estimated differential accelerometer error ({right arrow over (e)}) is determined by comparing the differential acceleration ({right arrow over (a)}diff) with an estimated differential acceleration determined based on an estimated attitude determined using TRIAD method. For each of a plurality of sequential iterations, adjustments to the combined-sensor conversion values (x) are determined based on the value of the estimated accelerometer error ({right arrow over (e)}) using the Gauss-Newton method (e.g., adjusting the combined-sensor conversion values in a way that will reduce the estimated accelerometer error ({right arrow over (e)}). The adjusted combined-sensor conversion values determined in the current iteration are used to generate values for estimated accelerometer error ({right arrow over (e)}) for the next iteration.
In some embodiments, when multiple accelerometer measurements acquired at different device orientations are used to calibrate the accelerometer, during a single iteration a different estimated accelerometer error ({right arrow over (e)}) is calculated for each accelerometer measurement of the multiple accelerometer measurements using the same set of combined-sensor conversion values (x), and the adjustments to the combined-sensor conversion values are determined for all of the accelerometer measurements in the multiple accelerometer measurements. In other words, each iteration includes determining an estimated accelerometer error ({right arrow over (e)}) for each accelerometer measurement and adjusting the shared combined-sensor conversion values (x) so as to minimize these estimated accelerometer errors, on average. Iterations are repeated until the combined-sensor conversion values produce an estimated accelerometer error that is sufficiently small (e.g., below a predefined threshold). Typically, combined-sensor conversion values that produce an acceptably small error can be generated with approximately 20-30 iterations. Performing additional iterations of the Gauss-Newton method will generally not increase the accuracy of the accelerometer after convergence has been reached (i.e., the error value (e) has reached a minimum). However, in some implementations fewer than 20-30 iterations of the Gauss-Newton method can be used if computational resources are scarce, as additional iterations increase the time and computational resources (memory, processing power, etc.) that are consumed by the calibration process. Thus, the number of iterations can be adjusted in accordance with the desired tradeoff between accuracy and speed/computational resources. It should be understood that while the Gauss-Newton estimation method is described as one possible approach for differential calibration of accelerometers, many other options exist, for example a Kalman filter could be used to iteratively estimate the combined-sensor conversion values for the accelerometer as each accelerometer measurement is received.
It should be understood that these combined-sensor conversion values are not generally used to directly determine a corrected acceleration of Device 102. This is because the combined-sensor conversion values indicate a relative calibration between two different accelerometers. In other words, the combined-sensor conversion values enable the two accelerometers to be calibrated relative to one another (e.g., “tuned” to each other), rather than providing information that, by itself, enables the accelerometers to be calibrated with respect to the surrounding environment. As an illustrative example, in a situation where the two accelerometers have identical characteristics and orientation within Device 102, the estimated differential accelerometer error ({right arrow over (e)}) would always be zero, because there is no difference between the accelerometers, and thus Dd and {right arrow over (b)}d would each be a null matrix (e.g., all of the combined-sensor conversion values (x) for Dd and {right arrow over (b)}d zero). In other words, each non-zero combined-sensor conversion value for equations 7-12 corresponds to a difference between the characteristics and/or orientation of the two accelerometers within Device 102. These combined-sensor conversion values can therefore be used to improve the accelerometer calibration described above with reference to Equations 5-6, as described in greater detail below with reference to Equations 10-12.
After calibrating the combined-sensor output, Device 102 adjusts (716) the calibration of the first accelerometer in accordance with the combined-sensor conversion values. In some embodiments, calibrating (718) the first accelerometer includes calibrating scale and/or offset of the first accelerometer (e.g., the diagonal elements of D1 and the elements of {right arrow over (b)}1, respectively in Equation 11) and adjusting the calibration of the first accelerometer includes adjusting the calibration of skew and/or rotation of the first accelerometer (e.g., by subtracting at least a portion of the off-diagonal elements of Dd from D1, as shown in Equation 11). Additionally, in some embodiments, Device 102 also adjusts (720) the calibration of the second accelerometer in accordance with the calibrated combined-sensor output. In some of these embodiments, calibrating (722) the second accelerometer includes calibrating scale and/or offset of the second accelerometer (e.g., the diagonal elements of D2 and the elements of {right arrow over (b)}2, respectively in Equation 12) and adjusting the calibration of the second accelerometer includes adjusting the calibration of skew and/or rotation of the second accelerometer (e.g., by subtracting at least a portion of the off-diagonal elements of Dd from D2, as shown in Equation 12).
In some embodiments, adjusting (724) the calibration of the first accelerometer includes adjusting a respective first-accelerometer conversion value in accordance with a particular combined-sensor conversion value (e.g., adding a multiple of the particular combined-sensor conversion value to the respective first-accelerometer conversion value). Additionally, in some of these embodiments, adjusting the calibration of the second accelerometer includes adjusting a respective second-accelerometer conversion value that corresponds to the respective first-accelerometer conversation value in accordance with the particular combined-sensor conversion value. (e.g., subtracting a multiple of the particular combined-sensor conversion value from the respective second-accelerometer conversion value), an example of adjusting the calibration of the first accelerometer in this way is described in greater detail below with reference to Equations 10-12.
In some embodiments, the combined-sensor conversion values are used to adjust the skew accelerometer conversion values of the individual accelerometers (e.g., the first accelerometer and/or the second accelerometer). When the skew accelerometer conversion values (e.g., the off diagonal terms in the matrix Dd) are to be adjusted and scale accelerometer conversion values do not need to be adjusted, the on-diagonal terms are removed from Dd (e.g., x4-x6 are set to zero) to generate an adjusted differential D matrix D′d. D′d is then used to augment the D matrix for the accelerometer (from Equation 5). The respective D matrices for the respective accelerometers are represented below as D1 (for the first accelerometer) and D2 (for the second accelerometer) and D2.
In Equation 11, half of each the off-diagonal terms from the differential calibration are subtracted from D1, while in Equation 12, half of each the off-diagonal terms from the differential calibration are added to D2. It should be understood that these updates to the D matrices (D1 and D2) are not based on any additional or more accurate information that would intrinsically improve the accuracy of the calibration, because these updates are based on the same accelerometer and magnetometer measurements have been used for all of the calibrations described above. Rather, the updates to the D matrices take into account the differences between the output of the two accelerometers, which typically produces a better estimate of the off-diagonal (skew) terms than estimating the off-diagonal terms directly, thereby averaging out any outlying skew terms. This formulation of the estimation problem provides good estimates of the off-diagonal terms because it is much less sensitive to errors in the device orientation (CTRIAD). In many non-differential accelerometer formulations, for a single accelerometer calibration, a small error in device orientation will produce a large error due to a misaligned gravity vector. In contrast, in the differential accelerometer formulation described above with reference to equations 7-12, these gravity vector misalignments cancel out.
It should be understood that the methods described above for calibrating multiple accelerometers by calibrating a combined-sensor output may be performed at a device that initially includes an uncalibrated magnetometer and where a calibrated magnetometer is used to determine the orientation of Device 102 using the TRIAD approach (e.g., the CTRIAD formula described above with reference to Equations 5-6). Thus, in some embodiments, Device 102 includes a magnetometer Device 102 calibrates a magnetometer (e.g., as described above with reference to Equation 4), where the magnetometer is calibrated using a set of measurements from a different plurality of sample orientations than the plurality of sample orientations used to calibrate the accelerometers (e.g., as described in greater detail above with reference to
It should be understood that the particular order in which the operations in
It is noted that in some of the embodiments described above, Device 102 does not include a gesture determination module 1119, because gesture determination is performed by Host 101. In some embodiments described above, Device 102 also does not include Kalman filter module 1120 because Device 102 transmits sensor measurements (e.g., accelerometer and magnetometer measurements) and, optionally, button presses 1116 to Host 101 at which a navigational state of Device 102 is determined.
Each of the above identified elements may be stored in one or more of the previously mentioned memory devices, and each of the above identified programs or modules corresponds to a set of instructions for performing a function described above. The set of instructions can be executed by one or more processors (e.g., CPUs 1102). The above identified modules or programs (i.e., sets of instructions) need not be implemented as separate software programs, procedures or modules, and thus various subsets of these modules may be combined or otherwise re-arranged in various embodiments. In some embodiments, Memory 1110 may store a subset of the modules and data structures identified above. Furthermore, Memory 1110 may store additional modules and data structures not described above.
Although
It is noted that in some of the embodiments described above, Host 101 does not store data representing Sensor Measurements 1217, and also does not include Kalman Filter Module 1220 because sensor measurements of Device 102 are processed at Device 102, which sends data representing Navigational State Estimate 1216 to Host 101. In other embodiments, Device 102 sends data representing Sensor Measurements 1217 to Host 101, in which case the modules for processing that data are present in Host 101.
Each of the above identified elements may be stored in one or more of the previously mentioned memory devices, and each of the above identified programs or modules corresponds to a set of instructions for performing a function described above. The set of instructions can be executed by one or more processors (e.g., CPUs 1202). The above identified modules or programs (i.e., sets of instructions) need not be implemented as separate software programs, procedures or modules, and thus various subsets of these modules may be combined or otherwise re-arranged in various embodiments. The actual number of processors and software modules used to implement Host 101 and how features are allocated among them will vary from one implementation to another. In some embodiments, Memory 1210 may store a subset of the modules and data structures identified above. Furthermore, Memory 1210 may store additional modules and data structures not described above.
Note that methods 500, 600 and 700 described above are optionally governed by instructions that are stored in a non-transitory computer readable storage medium and that are executed by one or more processors of Device 102 or Host 101. As noted above, in some embodiments these methods may be performed in part on Device 102 and in part on Host 101, or on a single integrated system which performs all the necessary operations. Each of the operations shown in
The foregoing description, for purpose of explanation, has been described with reference to specific embodiments. However, the illustrative discussions above are not intended to be exhaustive or to limit the invention to the precise forms disclosed. Many modifications and variations are possible in view of the above teachings. The embodiments were chosen and described in order to best explain the principles of the invention and its practical applications, to thereby enable others skilled in the art to best utilize the invention and various embodiments with various modifications as are suited to the particular use contemplated.
This application claims the benefit of U.S. Provisional Application Ser. No. 61/584,178, filed Jan. 6, 2012, which application is incorporated by reference herein in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
3953795 | Brunner et al. | Apr 1976 | A |
4263494 | Martin | Apr 1981 | A |
4318186 | Wynn | Mar 1982 | A |
4467272 | Hassler et al. | Aug 1984 | A |
4516770 | Brookes et al. | May 1985 | A |
4641246 | Halbert et al. | Feb 1987 | A |
4816748 | Tazawa et al. | Mar 1989 | A |
4847783 | Grace et al. | Jul 1989 | A |
4851775 | Kim et al. | Jul 1989 | A |
4964727 | Huggins | Oct 1990 | A |
5128671 | Thomas, Jr. | Jul 1992 | A |
5161311 | Esmer et al. | Nov 1992 | A |
5239264 | Hawks | Aug 1993 | A |
5321401 | White | Jun 1994 | A |
5637994 | Carder | Jun 1997 | A |
5645077 | Foxlin | Jul 1997 | A |
5757360 | Nitta et al. | May 1998 | A |
5819206 | Horton et al. | Oct 1998 | A |
5874941 | Yamada | Feb 1999 | A |
5893049 | Reggiardo | Apr 1999 | A |
6072467 | Walker | Jun 2000 | A |
6157894 | Hess et al. | Dec 2000 | A |
6176837 | Foxlin | Jan 2001 | B1 |
6243476 | Gardner | Jun 2001 | B1 |
6304828 | Swanick et al. | Oct 2001 | B1 |
6384596 | Beyer | May 2002 | B1 |
6593956 | Potts et al. | Jul 2003 | B1 |
6882086 | Kornbluh et al. | Apr 2005 | B2 |
7139983 | Kelts | Nov 2006 | B2 |
7154275 | Zank et al. | Dec 2006 | B2 |
7158118 | Liberty | Jan 2007 | B2 |
7216055 | Horton et al. | May 2007 | B1 |
7246058 | Burnett | Jul 2007 | B2 |
7262760 | Liberty | Aug 2007 | B2 |
7285964 | Hsu et al. | Oct 2007 | B1 |
7296363 | Danisch et al. | Nov 2007 | B2 |
7305630 | Hullender et al. | Dec 2007 | B2 |
7307411 | Hsu et al. | Dec 2007 | B1 |
7350303 | Rock et al. | Apr 2008 | B2 |
7414611 | Liberty | Aug 2008 | B2 |
7451549 | Sodhi et al. | Nov 2008 | B1 |
7647185 | Tarassenko et al. | Jan 2010 | B2 |
7815508 | Dohta | Oct 2010 | B2 |
7844415 | Bryant et al. | Nov 2010 | B1 |
7940986 | Mekenkamp et al. | May 2011 | B2 |
7978178 | Pehlivan et al. | Jul 2011 | B2 |
8184100 | Lian et al. | May 2012 | B2 |
8201200 | Imai | Jun 2012 | B2 |
8223121 | Shaw et al. | Jul 2012 | B2 |
8515707 | Joseph et al. | Aug 2013 | B2 |
8576169 | Shaw et al. | Nov 2013 | B2 |
8577677 | Kim et al. | Nov 2013 | B2 |
8587519 | Shaw et al. | Nov 2013 | B2 |
8712069 | Murgia et al. | Apr 2014 | B1 |
8787587 | Murgia et al. | Jul 2014 | B1 |
8907893 | Shaw et al. | Dec 2014 | B2 |
8957909 | Joseph et al. | Feb 2015 | B2 |
9152249 | Shaw et al. | Oct 2015 | B2 |
9228842 | Joseph et al. | Jan 2016 | B2 |
9316513 | Joseph et al. | Apr 2016 | B2 |
20020120217 | Adapathya et al. | Aug 2002 | A1 |
20020158815 | Zwern | Oct 2002 | A1 |
20020169553 | Perlmutter | Nov 2002 | A1 |
20030016835 | Elko et al. | Jan 2003 | A1 |
20030018430 | Ladetto et al. | Jan 2003 | A1 |
20030023192 | Foxlin | Jan 2003 | A1 |
20030107888 | Devlin et al. | Jun 2003 | A1 |
20030149907 | Singh et al. | Aug 2003 | A1 |
20030164739 | Bae | Sep 2003 | A1 |
20030169891 | Ryan et al. | Sep 2003 | A1 |
20040052391 | Bren et al. | Mar 2004 | A1 |
20040198463 | Knoedgen | Oct 2004 | A1 |
20040199674 | Brinkhus | Oct 2004 | A1 |
20050008169 | Muren et al. | Jan 2005 | A1 |
20050229117 | Hullender et al. | Oct 2005 | A1 |
20060033716 | Rosenberg et al. | Feb 2006 | A1 |
20060164384 | Smith et al. | Jul 2006 | A1 |
20060164386 | Smith et al. | Jul 2006 | A1 |
20060195254 | Ladetto et al. | Aug 2006 | A1 |
20060217977 | Gaeta et al. | Sep 2006 | A1 |
20060250358 | Wroblewski | Nov 2006 | A1 |
20070146319 | Masselle et al. | Jun 2007 | A1 |
20070234779 | Hsu et al. | Oct 2007 | A1 |
20070287911 | Haid et al. | Dec 2007 | A1 |
20080072234 | Myroup | Mar 2008 | A1 |
20080080789 | Marks et al. | Apr 2008 | A1 |
20080140338 | No et al. | Jun 2008 | A1 |
20080150891 | Berkley et al. | Jun 2008 | A1 |
20080173717 | Antebi et al. | Jul 2008 | A1 |
20080211768 | Breen et al. | Sep 2008 | A1 |
20080281555 | Godin et al. | Nov 2008 | A1 |
20080284729 | Kurtenbach et al. | Nov 2008 | A1 |
20090009471 | Yamamoto et al. | Jan 2009 | A1 |
20090040175 | Xu et al. | Feb 2009 | A1 |
20090048021 | Lian et al. | Feb 2009 | A1 |
20090055170 | Nagahama | Feb 2009 | A1 |
20090153349 | Lin et al. | Jun 2009 | A1 |
20090295722 | Yamamoto | Dec 2009 | A1 |
20090326857 | Mathews et al. | Dec 2009 | A1 |
20100039381 | Cretella, Jr. et al. | Feb 2010 | A1 |
20100060573 | Moussavi | Mar 2010 | A1 |
20100088061 | Horodezky | Apr 2010 | A1 |
20100095773 | Shaw et al. | Apr 2010 | A1 |
20100097316 | Shaw et al. | Apr 2010 | A1 |
20100110001 | Yamamoto | May 2010 | A1 |
20100123605 | Wilson | May 2010 | A1 |
20100123656 | Park et al. | May 2010 | A1 |
20100128881 | Petit et al. | May 2010 | A1 |
20100128894 | Petit et al. | May 2010 | A1 |
20100149341 | Marks et al. | Jun 2010 | A1 |
20100150404 | Marks et al. | Jun 2010 | A1 |
20100156786 | Kabasawa et al. | Jun 2010 | A1 |
20100157168 | Dunton et al. | Jun 2010 | A1 |
20100174506 | Joseph | Jul 2010 | A1 |
20100194879 | Pasveer et al. | Aug 2010 | A1 |
20100302145 | Langridge et al. | Dec 2010 | A1 |
20100315905 | Lee et al. | Dec 2010 | A1 |
20110163947 | Shaw et al. | Jul 2011 | A1 |
20110172918 | Tome | Jul 2011 | A1 |
20110205156 | Gomez et al. | Aug 2011 | A1 |
20110239026 | Kulik | Sep 2011 | A1 |
20110241656 | Piemonte et al. | Oct 2011 | A1 |
20110242361 | Kuwahara et al. | Oct 2011 | A1 |
20120007713 | Nasiri | Jan 2012 | A1 |
20120011351 | Mundra et al. | Jan 2012 | A1 |
20120058803 | Nicholson | Mar 2012 | A1 |
20120086725 | Joseph | Apr 2012 | A1 |
20120130667 | Fukushima | May 2012 | A1 |
20120268249 | Kansal et al. | Oct 2012 | A1 |
20130179108 | Joseph et al. | Jul 2013 | A1 |
20130192333 | Tohta | Aug 2013 | A1 |
20130253821 | Joseph et al. | Sep 2013 | A1 |
20130253880 | Joseph et al. | Sep 2013 | A1 |
20140055351 | Shaw et al. | Feb 2014 | A1 |
20140139432 | Shaw et al. | May 2014 | A1 |
20140149060 | Meduna et al. | May 2014 | A1 |
20160026265 | Shaw et al. | Jan 2016 | A1 |
Number | Date | Country |
---|---|---|
1762287 | Mar 2007 | EP |
2120134 | Nov 2009 | EP |
2120134 | Nov 2009 | EP |
2485119 | Aug 2012 | EP |
2485119 | Aug 2012 | EP |
2579127 | Apr 2013 | EP |
2579127 | Apr 2013 | EP |
WO2004047011 | Jun 2004 | WO |
WO2005040991 | May 2005 | WO |
WO2005040991 | May 2005 | WO |
WO2005108119 | Nov 2005 | WO |
WO2005108119 | Nov 2005 | WO |
WO2006054295 | May 2006 | WO |
WO2006054295 | May 2006 | WO |
WO2006090197 | Aug 2006 | WO |
WO2006090197 | Aug 2006 | WO |
WO2009093161 | Jul 2009 | WO |
WO2009132920 | Nov 2009 | WO |
WO2009156499 | Dec 2009 | WO |
WO2010048000 | Apr 2010 | WO |
WO2010048000 | Apr 2010 | WO |
WO2010080383 | Jul 2010 | WO |
WO2010080383 | Jul 2010 | WO |
WO2011085017 | Jul 2011 | WO |
WO2011109229 | Sep 2011 | WO |
WO2011109229 | Sep 2011 | WO |
WO2012047494 | Apr 2012 | WO |
WO2013104006 | Jul 2013 | WO |
WO2013104006 | Jul 2013 | WO |
WO2013148585 | Oct 2013 | WO |
WO2013148585 | Oct 2013 | WO |
WO2014085615 | Jun 2014 | WO |
Entry |
---|
International Search Report and Written Opinion for International Application No. PCT/US2009/060475 mailed May 18, 2010. 9 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2009/067976 mailed May 3, 2010. 9 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2011/020242 mailed Apr. 12, 2011. 13 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2011/052185 mailed Jan. 31, 2012. 11 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2012/020365 mailed May 23, 2012. 10 pages. |
International Search Report and Written Opinion for International Application No. PCT/US2013/033723 mailed Jul. 29, 2013. |
Sedlak et al., “Automated Attitude Sensor Calibration: Progress and Plans,” in Paper No. AIAA-2004-4854, AIAA/AAS Astrodynamics Specialist Conference, Aug. 2004, Providence, RI, vol. 2, No. 4 , 14 pages. |
Written Opinion mailed Nov. 30, 2011 in Patent Cooperation Treaty Application No. PCT/US2009/060475, filed Oct. 13, 2009. |
Ang, Wei Tech et al., “Kalman Filtering for Real-Time Orientation Tracking of Handheld Microsurgical Instrument,” Proceedings of 2004 IEEE/RSJ International Conference on Intelligent Robots and Systems; Sep. 28-Oct. 2, 2004; Sendai, Japan, pp. 2574-2580. |
International Search Report and Written Opinion mailed May 18, 2010 in Patent Cooperation Treaty Application No. PCT/US2009/060475, filed Oct. 13, 2009. |
International Search Report and Written Opinion mailed May 3, 2010 in Patent Cooperation Treaty Application No. PCT/US2009/067976, filed Dec. 15, 2009. |
Simon, D., “Kalman Filtering,” Embedded Systems Programming, vol. 14, No. 6, Jun. 2001, pp. 72-79. |
International Search Report and Written Opinion mailed Jan. 31, 2012 in Patent Cooperation Treaty Application No. PCT/US2011/052185. |
Foxlin, E., “Inertial Head-Tracker Sensor Fusion by a Complementary Separate-Bias Filter,” in Proceedings of the IEEE Virtual Reality Annual International Symposium, 1996, pp. 185-195. |
Foxlin et al., “Miniature 6-DOF Inertial System for Tracking HMDs,” in SPIE, vol. 3362, Helmet and Head—Mounted Displays, III, AeroSense 98, Orlando, FL, Apr. 13-14, 1998, pp. 1-15. |
International Search Report and Written Opinion mailed Jul. 29, 2013 in Patent Cooperation Treaty Application No. PCT/US2013/033723, filed Mar. 25, 2013. |
Sedlak, J. “Spinning Spacecraft Attitude Estimation Using Markley Variables: Filter Implementation and Results,” NASA Goddard Space Flight Center CP-2005-212789, Greenbelt, MD (2005), 15 pages. |
Luong-Van et al. “Covariance Profiling for an Adaptive Kalman Filter to Suppress Sensor Quantization Effects,” 43rd IEEE Conference on Decision and Control, vol. 3, Dec. 14-17, 2004, pp. 2680-2685. |
International Search Report and Written Opinion mailed Dec. 19, 2014 in Patent Cooperation Treaty Application No. PCT/US2013/072278 mailed Dec. 19, 2014. |
Wang et al., “A Framework of Energy Efficient Mobile Sensing for Automatic User State Recognition,” Proceedings of the 7th International Conference on Mobile Systems, Applications, and Services, MOBISYS '09, Jun. 2009, pp. 179-192. |
Girod et al., “The Design and Implementation of a Self-Calibrating Distributed Acoustic Sensing Platform,” SenSys 06, Nov. 1-3, 2006, 14 pages. |
Kim et al., “Modeling and Calibration of a Multi-Spectral Imaging Sensor for In-Field Crop Nitrogen Assessment,” Applied Engineering in Agriculture, vol. 22, No. 6, Sep. 2006, pp. 935-941. |
Ramanathan et al., “Rapid Deployment with Confidence: Calibration and Fault Detection in Environmental Sensor Networks,” Center for Embedded Networked Sensing, UCLA, Department of Civil and Environmental Engineering, MIT, Jul. 4, 2006, pp. 1-14. |
Bychkovskiy, Vladimir Leonidovich, “Distributed In-Place Calibration in Sensor Networks,” University of California Master of Science in Computer Science Thesis, 2003. 42 pages. |
Sedlak et al., “Automated Attitude Sensor Calibration: Progress and Plans,” in Paper No. AIAA-2004-4854, AIAA/AAS Astrodynamics Specialist Conference, Aug. 2004, Providence, RI, vol. 2, No. 4, 14 pages. |
International Search Report and Written Opinion mailed Sep. 13, 2013 in Patent Cooperation Treaty Application No. PCT/US2013/020687, filed Jan. 8, 2013. |
International Search Report and Written Opinion mailed Nov. 30, 2011 in Patent Cooperation Treaty Application No. PCT/US2009/060475, filed Oct. 13, 2009. |
Number | Date | Country | |
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20130174636 A1 | Jul 2013 | US |
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61584178 | Jan 2012 | US |