Xivanki Share !!: Example application for accelerometer/compass processing on Android

Example application for accelerometer/compass processing on Android - Selamat datang di situs media global terbaru Xivanki, Pada halaman ini kami menyajikan informasi tentang Example application for accelerometer/compass processing on Android !! Semoga tulisan dengan kategori ini bermanfaat bagi anda. Silahkan sebarluaskan postingan Example application for accelerometer/compass processing on Android ini ke social media anda, Semoga rezeki berlimpah ikut dimudahkan Allah bagi anda, Lebih jelas infonya lansung dibawah -->

I hope you are well prepared by now what you can expect from the compass-accelerometer sensor fusion - if not, please read my thoughts about the limitations. This time we are going to see, how to compensate the accelerometer with the compass.

The idea is very simple. The accelerometer and the compass both measure vectors fixed to the Earth. These vectors are different - gravity and ambient magnetic field - but we hope that their angle is constant because they are both fixed to the same coordinate system. But while the accelerometer is sensitive to the motion acceleration, the compass is not. If we manage to rotate and scale the magnetic field vector into the gravity vector, we have a reference while the accelerometer is subject to motion acceleration and we can extract the motion acceleration. Plus, we have a reliable gravity vector and an "in motion" indication.

So the process is the following:

• Calibrate the compass to the location and figure out the offsets we discussed in the limitation part. Also measure the reference gravity vector length.
• If we find that the acceleration vector's length is close enough to the reference gravity vector length, we assume that this means "no motion" (see the discussion of this issue here). Find then the rotation axis and angle to rotate the compass vector into the acceleration vector. We call these values reference rotation axis, reference rotation angle, reference magnetic vector and reference acceleration vector, respectively. Keep updating these values as long as we are in "no motion" state.
  
• If we find, that the acceleration vector's length is significantly shorter or longer than the reference gravity vector length, we are in "motion" state. Then we use the previously recorded reference values and the actual magnetic field value measured by the compass to calculate a simulated gravity vector. Using the measured acceleration vector and the simulated gravity vector, we extract the motion acceleration vector.

Simple, isn't it? Yes, it is, the only part requiring attention is the rotation bit. The task is the following: we have a reference magnetic vector and a reference acceleration vector from an earlier measurement. Then the acceleration vector length was close to reference gravity so we can assume that the reference acceleration vector mostly contains gravity component. Now we have a current magnetic vector and a current acceleration vector. The acceleration vector, however, seems to contain motion acceleration component too. How to simulate a gravity vector from the current magnetic vector?

The steps are:

• Calculate the rotation operation that rotates the reference magnetic vector to the reference acceleration vector. The rotation operation has two components: an axis around which one vector is rotated to the other and a rotation angle. The rotation axis is the vector cross product of the two vectors. The angle can be obtained by resolving the equation of two different representations of the two vectors' dot product. This yields reference rotation axis and reference rotation angle.
  
• The reference rotation axis nicely rotates the reference magnetic vector to the reference acceleration vector but we need to apply the rotation to the current magnetic vector. We need a new rotation axis for this and we obtain it by rotating the reference rotation axis by the rotation operation that rotates reference magnetic vector to the current magnetic vector. This yields a current rotation axis.
• Then we simply rotate the current magnetic vector around the current rotation axis with the reference rotation angle. This yields a simulated gravity vector. We also have to scale this vector so that its length is equal to the reference gravity.

Once we are done with this, we can subtract the simulated gravity vector from the current acceleration vector and we have the motion acceleration.

Let's see the example Android program then that implements all this!

The example program can be downloaded from here.

The program is really just a variation of the gyroscope/accelerometer example program. The main difference is that when the sampling is started, you have to calibrate the compass first. The application instructs you, which edge/side of the device should be turned toward the Earth and the calibration steps already passed disappear from the screen. This is really a major annoyance compared to the gyroscope version but that's the price we pay for having a widely available sensor instead of the rare gyroscope.

After the calibration you see the familiar ball that visualizes the measured motion acceleration (the size of the ball is proportional with the z component of the motion acceleration). As with the gyroscope case, the motion acceleration is rotated into the Earth's coordinate system. If you need the motion acceleration in the device's coordinate system, just remove the rotateToEarth() method invocation.

If you set DEBUG to true in SamplingService.java, the program creates a (potentially large) file containing measurement data as /sdcard/capture.csv. You can analyze it with this Sage script.

Now we have two methods of extracting motion acceleration. The gyroscope is more convenient because it is not subject to external magnetic fields or metal objects but is available in less devices. There are more hassles with the compass but at the end it works nicely too. The next step is to recognize movement patterns in the 3D motion acceleration vectors.