# Implementing Positioning Algorithms Using Accelerometers

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1 Freescale Semiconductor Application Note Rev 0, 02/2007 Implementing Positioning Algorithms Using Accelerometers by: Kurt Seifert and Oscar Camacho OVERVIEW This document describes and implements a positioning algorithm using the MMA7260QT 3-Axis accelerometer and a 9S08QG8 low cost 8-bit microcontroller unit (MCU). In today s advanced electronic market, there are many multifunctional products continuously adding features and intelligence. Tracking and gaming are just a few of the markets that can benefit from obtaining positioning information. One option for obtaining this information is through the use of inertial sensors. The signal obtained from these sensors does require processing as there is no direct conversion between acceleration and position. In order to obtain position a double integral must be applied to the signal. This document describes an easy algorithm to implement a double integration of the signal obtained from the sensor using a low end 8-bit microcontroller. In order to obtain a double integration a simple integration must be made twice. This allows velocity information to be obtained as well. The algorithm shown in the following pages applies to any sensing axis; therefore, one, two or three dimensional positioning can be determined. When implementing positioning in 3 axes, extra processing is required to null the earth s gravity effect. The implementation below includes an example for a 2-axis system (i.e. mouse). POTENTIAL APPLICATIONS Potential applications for this kind of algorithm are personal navigation, car navigation, back-up GPS, anti-theft devices, map tracking, 3-D gaming, PC mouse, plus many others. The products in these categories can benefit from implementing positioning algorithms. The algorithm described in this document is useful in situations where displacement precision is not extremely critical. Other considerations and implications specific to the application should be considered when adapting this example. With minor modifications and adaptations in the final application this algorithm can achieve higher precision. BACK UP THEORY AND ALGORITHM The best approach in understanding this algorithm is with a review of mathematical integration. The acceleration is the rate of change of the velocity of an object. At the same time, the velocity is the rate of change of the position of that same object. In other words, the velocity is the derivative of the position and the acceleration is the derivative of the velocity, thus: dv a ds = and v dds ( ) = a = dt dt dt 2 The integration is the opposite of the derivative. If the acceleration of an object is known, we can obtain the position data if a double integration is applied (assuming initial conditions are zero): v = ( a ) d t and s= ( v) dt ( a) dt dt One way to understand this formula is to define the integral as the area below the curve, where the integration is the sum of very small areas whose width is almost zero. In other words, the sum of the integration represents the magnitude of a physical variable. Figure 1. Sampled Accelerometer s Signal Where: b n ƒ( x) dx = a lim ƒ( x i ) n x i = 1 b a x = n Freescale Semiconductor, Inc., All rights reserved.

2 With the previous concept about areas below the curve a deduction can be made: Sampling a signal gets us instant values of its magnitude, so small areas can be created between two samples. In order to create a coherent value, sampling time must always be the same. Sampling time represents the base of this area while the sampled value represents its height. In order to eliminate multiplications with fractions (microseconds or milliseconds) involving floating points in the calculation we assume the time is a unit. Now we know each sample represents an area whose base width is equal to 1. The next deduction could then be that the value of the integral is reduced to be the sum of samples. This assumption is correct if the sampling time tends to be zero. In a real situation an error is generated as shown in Figure 1. This error keeps accumulating for the time the process is active. Area error Formula 1 Sample n Sample n 1 Area n = Sample n T 2 Now the error is much lower than in the previous approximation. Yet data must not be too accurate in order to obtain a real world interpretation. Even though acceleration can be positive or negative, samples are always positive (based on the output characteristics of the MMA7260QT); therefore, an offset adjustment must be done. In other words, a reference is needed. This function is defined as the calibration routine. Calibration is performed on the accelerometer when there is a no movement condition. The output or offset obtained is considered the zero point reference. Values lower than the reference represent negative values (deceleration) while greater values represent positive values (acceleration). The accelerometer output varies from 0V to Vdd and it is typically interpreted by an analog to digital comparator (A/D). The zero value is near Vdd/2. The calibration value obtained will be affected by the board s orientation and the static acceleration (earth s gravity) component in each of the axis. If the module is perfectly parallel to the earth s surface, the calibration value should be very close to Vdd/2. The following figure shows the result of the calibration routine: Figure 2. Errors Generated During Integration These errors are formally known as sampling losses. In order to reduce this error we then make a further assumption. The resulting area can be seen as the combination of two smaller areas: Area 2 Area 1 Sampled Signal minus Zero Reference equals Real Sampled Acceleration Figure 4. Acceleration Signal After Calibration From the sampled signal minus the zero reference we obtain true sampled acceleration. A1 represents a positive acceleration. A2 represents a negative acceleration. If we considered this data as sampled data, the signal should be similar to the figure below. Sample n Sample n-1 Figure 3. Errors of Integration Are Reduced with a First Order Approximation (Trapezoidal Method) The first area is the value of the previous sample (a square). The second area is a triangle, formed between the previous sample (sample n-1) and the actual sample (sample n) divided by two. With this approach, we now have a first order approximation (interpolation) of the signal. Threshold Value A1 A2 Figure 5. Acceleration Sampled Signal After Calibration By applying the integration formula, Formula 1, we get a proportional approximation of the velocity. In order to obtain position the integration must be performed again. Applying the same formula and procedure to this obtained velocity data, we now get a proportional approximation of the instantaneous position (see Figure 6). 2 Freescale Semiconductor

3 Acceleration Velocity Position A) Real accelerometer data B) Result of the first Integration velocity C) Result of the second Integration velocity Figure 6. Proportional Approximation of the Instantaneous Position SOFTWARE DESIGN CONSIDERATIONS The following steps and recommendations should be considered when implementing this kind of algorithm in a real world implementation. The signal is not noise free so it must be digitally filtered. The filter used in this algorithm is a moving average; the value to be processed is the result of averaging a certain amount of samples. Even with the previous filtering some data can be erroneous due to the mechanical noise, so another filter must be implemented. Depending on the number of samples filtered, a window of real acceleration can be selected (typically ± 2 sample steps for an average of 16 samples). A no movement state is critical to obtain correct data. A calibration routine is needed at the beginning of the application. This calibration value must be as accurate as possible. The real value of the acceleration is the sample minus the calibration value; it can be either positive or negative. This must never be ignored when declaring variables (signed). A faster sampling frequency implies more accurate results due the fact that error is reduced; yet more memory, timing, and hardware considerations are needed. The time between samples MUST always be the same. Errors can be generated if this time is not equal. A linear approximation between samples (interpolation) is recommended for more accurate results. Freescale Semiconductor 3

4 Calibration Routine: CODE EXPLANATION This calibration routine removes the acceleration offset component in the sensor output due to the earth s gravity (static acceleration). The calibration routine averages samples when the accelerometer is in a no movement condition. The more samples that are taken, the more accurate the calibration results will be. void Calibrate(void) unsigned int count1; count1 = 0; do ADC_GetAllAxis(); sstatex = sstatex + Sample_X; sstatey = sstatey + Sample_Y; count1++; while(count1!=0x0400); // Accumulate Samples // 1024 times sstatex=sstatex>>10; // division between 1024 sstatey=sstatey>>10; Filtering: Low pass filtering of the signal is a very good way to remove noise (both mechanical and electrical) from the accelerometer. Reducing the noise is critical for a positioning application in order to reduce major errors when integrating the signal. A simple way for low pass filtering a sampled signal is to perform a rolling average. Filtering is simply then reduced to obtain the average of a set of samples. It is important to obtain the average of a balanced amount of samples. Taking too many samples to do this process can result in a loss of data, yet taking too few can result in an inaccurate value. do accelerationx[1]=accelerationx[1] + Sample_X; //filtering routine for noise attenuation accelerationy[1]=accelerationy[1] + Sample_Y; //64 samples are averaged. The resulting count2++; // average represents the acceleration of // an instant. while (count2!=0x40); // 64 sums of the acceleration sample accelerationx[1]= accelerationx[1]>>6; // division by 64 accelerationy[1]= accelerationy[1]>>6; Mechanical Filtering Window: When a no movement condition is present, minor errors in acceleration could be interpreted as a constant velocity due to the fact that samples not equal to zero are being summed; the ideal case for a no movement condition is all the samples to be zero. That constant velocity indicates a continuous movement condition and therefore an unstable position. Even with the previous filtering some data can be erroneous, so a window of discrimination between valid data and invalid data for the no movement condition must be implemented. if ((accelerationx[1] <=3)&&(accelerationx[1] >= -3)) //Discrimination window applied to accelerationx[1] = 0; // the X axis acceleration variable 4 Freescale Semiconductor

5 Figure 7. Software Discrimination Window To Reduce Mechanical Noise Effects Positioning: Double integration is the process needed to obtain the position using the acceleration data. The integration step must be performed once to obtain velocity and then repeated to obtain position. As previously shown: Sample n Sample n 1 Area n = Sample n T 2 //first integration velocityx[1] = velocityx[0] + accelerationx[0] + ((accelerationx[1] - accelerationx[0])>>1) //second integration positionx[1] = positionx[0] + velocityx[0] + ((velocityx[1] - velocityx[0])>>1); Data Transfer: This function is used for debugging and display purposes; the 32 bits result is split and conditioned in this function. if (positionx[1]>=0) //This line compares the sign of the X direction data direction= (direction 0x10); // if its positive the most significant byte posx_seg[0]= positionx[1] & 0x000000FF; // is set to 1 else it is set to 8 posx_seg[1]= (positionx[1]>>8) & 0x000000FF; // the data is also managed in the // subsequent lines in order to be sent. posx_seg[2]= (positionx[1]>>16) & 0x000000FF;// The 32 bit variable must be split into posx_seg[3]= (positionx[1]>>24) & 0x000000FF;// 4 different 8 bit variables in order to // be sent via the 8 bit SCI frame else direction=(direction 0x80); positionxbkp=positionx[1]-1; positionxbkp=positionxbkp^0xffffffff; posx_seg[0]= positionxbkp & 0x000000FF; posx_seg[1]= (positionxbkp>>8) & 0x000000FF; posx_seg[2]= (positionxbkp>>16) & 0x000000FF; posx_seg[3]= (positionxbkp>>24) & 0x000000FF; Freescale Semiconductor 5

6 Movement End Check Based on the concept that an integral represents the area below the curve, velocity is the result of the area below the acceleration curve. If we look at the typical movement of an object from point A to point B in a single axis, a typical acceleration would result as shown in the figure below: Acceleration Figure 8. Typical Accelerometer Output Signal As The Result of Dragging an Object in a Single Axis Looking at graph above, there is an initial acceleration or deceleration until a maximum velocity is reached. Then that acceleration flips the opposite way until it reaches zero again. At this point a stable displacement and a new position are reached. In a real world scenario where the area below the positive side of the curve is not the same as the area above the negative side, the integration result would never reach a zero velocity and therefore would be a sloped positioning (never stable). Because of this, it is crucial to force the velocity down to zero. This is achieved by constantly reading the acceleration and comparing it with zero. If this condition exists during a certain number of samples, velocity is simply returned to zero. if (accelerationx[1]==0) countx++; else countx =0; if (countx>=25) velocityx[1]=0; velocityx[0]=0; // we count the number of acceleration samples that equals cero // if this number exceeds 25, we can assume that velocity is cero 6 Freescale Semiconductor

7 Begin ADC Init Average Save X Offset Average Save Y Offset Y Calibrate? Take Sample From ADC N Acceleration = Sample calibration value Velocity = Previous Velocity + Current Acceleration Position = Previous Position + Current Velocity Show position SOURCE CODE #include <hidef.h> #include "derivative.h" #include "adc.h" #include "buzzer.h" #include "SCItx.h" Figure 9. Flow Diagram #pragma DATA_SEG MY_ZEROPAGE unsigned char near Sample_X; unsigned char near Sample_Y; unsigned char near Sample_Z; unsigned char near Sensor_Data[8]; unsigned char near countx,county ; signed int near accelerationx[2], accelerationy[2]; signed long near velocityx[2], velocityy[2]; signed long near positionx[2]; signed long near positiony[2]; signed long near positionz[2]; unsigned char near direction; unsigned long near sstatex,sstatey; #pragma DATA_SEG DEFAULT void init(void); void Calibrate(void); void data_transfer(void); Freescale Semiconductor 7

8 void concatenate_data(void); void movement_end_check(void); void position(void); void main (void) init(); get_threshold(); do position(); while(1); /******************************************************************************* The purpose of the calibration routine is to obtain the value of the reference threshold. It consists on a 1024 samples average in no-movement condition. ********************************************************************************/ void Calibrate(void) unsigned int count1; count1 = 0; do ADC_GetAllAxis(); sstatex = sstatex + Sample_X; sstatey = sstatey + Sample_Y; count1++; while(count1!=0x0400); // Accumulate Samples // 1024 times sstatex=sstatex>>10; // division between 1024 sstatey=sstatey>>10; /*****************************************************************************************/ /****************************************************************************************** This function obtains magnitude and direction In this particular protocol direction and magnitude are sent in separate variables. Management can be done in many other different ways. *****************************************************************************************/ void data_transfer(void) signed long positionxbkp; signed long positionybkp; unsigned int delay; unsigned char posx_seg[4], posy_seg[4]; if (positionx[1]>=0) //This line compares the sign of the X direction data direction= (direction 0x10); //if its positive the most significant byte posx_seg[0]= positionx[1] & 0x000000FF; // is set to 1 else it is set to 8 posx_seg[1]= (positionx[1]>>8) & 0x000000FF; // the data is also managed in the // subsequent lines in order to posx_seg[2]= (positionx[1]>>16) & 0x000000FF; // be sent. The 32 bit variable must be posx_seg[3]= (positionx[1]>>24) & 0x000000FF; // split into 4 different 8 bit // variables in order to be sent via // the 8 bit SCI frame 8 Freescale Semiconductor

9 else direction=(direction 0x80); positionxbkp=positionx[1]-1; positionxbkp=positionxbkp^0xffffffff; posx_seg[0]= positionxbkp & 0x000000FF; posx_seg[1]= (positionxbkp>>8) & 0x000000FF; posx_seg[2]= (positionxbkp>>16) & 0x000000FF; posx_seg[3]= (positionxbkp>>24) & 0x000000FF; if (positiony[1]>=0) // Same management than in the previous case direction= (direction 0x08); // but with the Y data. posy_seg[0]= positiony[1] & 0x000000FF; posy_seg[1]= (positiony[1]>>8) & 0x000000FF; posy_seg[2]= (positiony[1]>>16) & 0x000000FF; posy_seg[3]= (positiony[1]>>24) & 0x000000FF; else direction= (direction 0x01); positionybkp=positiony[1]-1; positionybkp=positionybkp^0xffffffff; posy_seg[0]= positionybkp & 0x000000FF; posy_seg[1]= (positionybkp>>8) & 0x000000FF; posy_seg[2]= (positionybkp>>16) & 0x000000FF; posy_seg[3]= (positionybkp>>24) & 0x000000FF; delay = 0x0100; Sensor_Data[0] = 0x03; Sensor_Data[1] = direction; Sensor_Data[2] = posx_seg[3]; Sensor_Data[3] = posy_seg[3]; Sensor_Data[4] = 0x01; Sensor_Data[5] = 0x01; Sensor_Data[6] = END_OF_FRAME; while (--delay); SCITxMsg(Sensor_Data); while (SCIC2 & 0x08); // Data transferring function /*****************************************************************************************/ /****************************************************************************************** This function returns data format to its original state. When obtaining the magnitude and direction of the position, an inverse two's complement is made. This function makes the two's complement in order to return the data to it original state. It is important to notice that the sensibility adjustment is greatly impacted here, the amount of "ones" inserted in the mask must be equivalent to the "ones" lost in the shifting made in the previous function upon the sensibility modification. ******************************************************************************************/ void data_reintegration(void) if (direction >=10) Freescale Semiconductor 9

10 positionx[1]= positionx[1] 0xFFFFC000; //amount of shifts // 18 "ones" inserted. Same size as the direction = direction & 0x01; if (direction ==1) positiony[1]= positiony[1] 0xFFFFC000; /****************************************************************************************** This function allows movement end detection. If a certain number of acceleration samples are equal to zero we can assume movement has stopped. Accumulated Error generated in the velocity calculations is eliminated by resetting the velocity variables. This stops position increment and greatly eliminates position error. ******************************************************************************************/ void movement_end_check(void) if (accelerationx[1]==0) countx++; else countx =0; if (countx>=25) velocityx[1]=0; velocityx[0]=0; //we count the number of acceleration samples that equals cero //if this number exceeds 25, we can assume that velocity is cero if (accelerationy[1]==0) county++; else county =0; //we do the same for the Y axis if (county>=25) velocityy[1]=0; velocityy[0]=0; /*****************************************************************************************/ /****************************************************************************************** This function transforms acceleration to a proportional position by integrating the acceleration data twice. It also adjusts sensibility by multiplying the "positionx" and "positiony" variables. This integration algorithm carries error, which is compensated in the "movenemt_end_check" subroutine. Faster sampling frequency implies less error but requires more memory. Keep in mind that the same process is applied to the X and Y axis. *****************************************************************************************/ void position(void) unsigned char count2 ; count2=0; do ADC_GetAllAxis(); accelerationx[1]=accelerationx[1] + Sample_X; //filtering routine for noise attenuation accelerationy[1]=accelerationy[1] + Sample_Y; //64 samples are averaged. The resulting 10 Freescale Semiconductor

11 //average represents the acceleration of //an instant count2++; while (count2!=0x40); // 64 sums of the acceleration sample accelerationx[1]= accelerationx[1]>>6; // division by 64 accelerationy[1]= accelerationy[1]>>6; accelerationx[1] = accelerationx[1] - (int)sstatex; //eliminating zero reference //offset of the acceleration data accelerationy[1] = accelerationy[1] - (int)sstatey; // to obtain positive and negative //acceleration if ((accelerationx[1] <=3)&&(accelerationx[1] >= -3)) //Discrimination window applied accelerationx[1] = 0; // to the X axis acceleration //variable if ((accelerationy[1] <=3)&&(accelerationy[1] >= -3)) accelerationy[1] = 0; //first X integration: velocityx[1]= velocityx[0]+ accelerationx[0]+ ((accelerationx[1] -accelerationx[0])>>1); //second X integration: positionx[1]= positionx[0] + velocityx[0] + ((velocityx[1] - velocityx[0])>>1); //first Y integration: velocityy[1] = velocityy[0] + accelerationy[0] + ((accelerationy[1] -accelerationy[0])>>1); //second Y integration: positiony[1] = positiony[0] + velocityy[0] + ((velocityy[1] - velocityy[0])>>1); accelerationx[0] = accelerationx[1]; //The current acceleration value must be sent //to the previous acceleration accelerationy[0] = accelerationy[1]; //variable in order to introduce the new //acceleration value. velocityx[0] = velocityx[1]; velocityy[0] = velocityy[1]; //Same done for the velocity variable positionx[1] = positionx[1]<<18; //is a sensibility adjustment. positiony[1] = positiony[1]<<18; //particular situation data_transfer(); positionx[1] = positionx[1]>>18; positiony[1] = positiony[1]>>18; //The idea behind this shifting (multiplication) //Some applications require adjustments to a //i.e. mouse application //once the variables are sent them must return to //their original state movement_end_check(); positionx[0] = positionx[1]; positiony[0] = positiony[1]; //actual position data must be sent to the //previous position direction = 0; // data variable to direction variable reset /*****************************************************************************************/ Freescale Semiconductor 11

12 SCHEMATIC CONCLUSIONS This application note provides the basic concepts for implementing a positioning algorithm using accelerometers. This specific algorithm is useful in situations where displacement precision is not extremely critical. Other considerations and implications specific to the application should be considered when implementing this example application. This integration algorithm is suitable for low end embedded applications because of its simplicity and small amount of instructions. It also does not involve any floating point calculations. REFERENCES Refer to the following documents for product information MC9S08QG8 Technical Data Sheet MMA7260Q Technical Data Sheet 12 Freescale Semiconductor

13 How to Reach Us: Home Page: Web Support: USA/Europe or Locations Not Listed: Freescale Semiconductor, Inc. Technical Information Center, EL East Elliot Road Tempe, Arizona or Europe, Middle East, and Africa: Freescale Halbleiter Deutschland GmbH Technical Information Center Schatzbogen Muenchen, Germany (English) (English) (German) (French) Japan: Freescale Semiconductor Japan Ltd. Headquarters ARCO Tower 15F 1-8-1, Shimo-Meguro, Meguro-ku, Tokyo Japan or Asia/Pacific: Freescale Semiconductor Hong Kong Ltd. Technical Information Center 2 Dai King Street Tai Po Industrial Estate Tai Po, N.T., Hong Kong For Literature Requests Only: Freescale Semiconductor Literature Distribution Center P.O. Box 5405 Denver, Colorado or Fax: Information in this document is provided solely to enable system and software implementers to use Freescale Semiconductor products. There are no express or implied copyright licenses granted hereunder to design or fabricate any integrated circuits or integrated circuits based on the information in this document. Freescale Semiconductor reserves the right to make changes without further notice to any products herein. Freescale Semiconductor makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does Freescale Semiconductor assume any liability arising out of the application or use of any product or circuit, and specifically disclaims any and all liability, including without limitation consequential or incidental damages. Typical parameters that may be provided in Freescale Semiconductor data sheets and/or specifications can and do vary in different applications and actual performance may vary over time. All operating parameters, including Typicals, must be validated for each customer application by customer s technical experts. Freescale Semiconductor does not convey any license under its patent rights nor the rights of others. Freescale Semiconductor products are not designed, intended, or authorized for use as components in systems intended for surgical implant into the body, or other applications intended to support or sustain life, or for any other application in which the failure of the Freescale Semiconductor product could create a situation where personal injury or death may occur. Should Buyer purchase or use Freescale Semiconductor products for any such unintended or unauthorized application, Buyer shall indemnify and hold Freescale Semiconductor and its officers, employees, subsidiaries, affiliates, and distributors harmless against all claims, costs, damages, and expenses, and reasonable attorney fees arising out of, directly or indirectly, any claim of personal injury or death associated with such unintended or unauthorized use, even if such claim alleges that Freescale Semiconductor was negligent regarding the design or manufacture of the part. Freescale and the Freescale logo are trademarks of Freescale Semiconductor, Inc. All other product or service names are the property of their respective owners. Freescale Semiconductor, Inc All rights reserved. Rev. 0 02/2007

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