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UWE Bristol Engineering showcase 2015

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Patrick Busch<br />

MEng Aerospace <strong>Engineering</strong> (Systems <strong>Engineering</strong>)<br />

Project Supervisor<br />

Dr. Chris Toomer<br />

Correction, calibration and evaluation of real measured data of<br />

aeroplane behaviour<br />

Introduction<br />

This study is the third in a series of masters´ theses<br />

on the topic of position, attitude and control input<br />

measurement during flight, particularly during spin<br />

of aircraft. This master´s thesis is designed to assist<br />

the PhD thesis of Steffen Schrader (University of<br />

Applied Sciences Osnabrueck) on the topic of spin<br />

prediction and simulation.<br />

Spinning<br />

Spin is a flight mode that can be referred to as<br />

autorotation around a vertical axis on a downward<br />

path. In order to enter a spin<br />

the aeroplane must be stalled<br />

and at the same time have a<br />

sufficient yaw rate or sideslip<br />

angle. When a stall occurs,<br />

the critical angle of attack<br />

is exceeded and the airflow<br />

over the wing is separated<br />

and becomes turbulent. The<br />

lift produced decreases<br />

Fig. 1: Spin<br />

considerably and hence the equilibrium of forces is<br />

unbalanced. Due to the mentioned sideslip angle<br />

or yaw rate, one wing will be stalled more than the<br />

other, resulting in a lower lift force and hence the<br />

aeroplane will start to roll in the direction of the<br />

more stalled wing. As a result from this rolling<br />

motion, a pitching and yawing moment will be<br />

induced. The drag on the more stalled wing will<br />

increase and support the rotation around the<br />

vertical axis as the aeroplane descends rapidly.<br />

Principle of Measurement<br />

To obtain position and attitude information of an<br />

aeroplane during every moment of its flight, the<br />

acceleration, measured on three axes by<br />

accelerometers, is integrated twice and the<br />

angular rate, measured around three axes by a<br />

gyroscope, is integrated once.<br />

Using the equations of motion the velocity and<br />

displacement can be calculated from the<br />

acceleration:<br />

v=∫a dt<br />

r=∫v dt<br />

And attitude is calculated from angular rate:<br />

θ=∫α dt<br />

Sentio32<br />

The measurement system implemented to record<br />

accelerations and angular<br />

rates basically consists of<br />

the Sentio32 platform and<br />

a Motion Sensor Board,<br />

which contains the actual<br />

gyroscopes and<br />

accelerometers. The Mid Fig. 2: Sentio32<br />

Sweden University designed the Sentio32<br />

hardware platform to provide a compact wireless<br />

sensor network platform that is IEEE802.15.4<br />

standard compatible and provides a high<br />

performance on local processing power. The<br />

sensors used during the measurements regarding<br />

this investigation are the capacitive 3D<br />

accelerometer KXSD9-2520 manufactured by<br />

KIONIX and two gyroscopes made by InvenSense,<br />

the IDG500 and the ISZ500.<br />

Statistical Analysis<br />

In order to obtain optimum results a universe of<br />

50 measurements was build and a statistical<br />

analysis was performed. From this data calibration<br />

curves were elaborated.<br />

Fig. 3: Statistical Analysis<br />

In order to verify the capabilities of the sensor in<br />

the second phase of the thesis flight test were<br />

conducted in two airplanes.<br />

Fig. 4: Test Aircraft, Citabria and Cessna C150<br />

Basic flight test were conducted in the C150, those<br />

consisted of rolling, pitching and yawing the<br />

airplane. Finally actual spin tests were conducted<br />

in the approved Citabria Campion.<br />

Examples of the recorded data are shown in the<br />

following figures.<br />

The cockpit<br />

instuments were<br />

captured during<br />

the basic flight<br />

tests to have a<br />

refference when<br />

evaluating the<br />

sensor data. For<br />

the spin tests an<br />

outside<br />

reference was<br />

required.<br />

Fig. 5: Inflight recordings<br />

The result, a complete recording of a spin can be<br />

seen in Fig. 6 below.<br />

Fig. 3: complete spin recording<br />

Project Summary<br />

This thesis deals with the improvement of a low-cost<br />

inertial measurement unit (IMU) for aeroplanes,<br />

which is already implemented in the Sentio32<br />

hardware platform and mounted to a 4-seated<br />

general aviation aeroplane. The correction as well as<br />

the calibration of the measured data, is the main<br />

topic of this project. The basic errors of the<br />

accelerometers and gyroscopes are elaborated based<br />

on a static test and can be traced back to a random<br />

offset of the accelerometer data and a linear drift in<br />

the angular rates. Different correction methods are<br />

applied based on a calibration curve derived from a<br />

set of measurements or a trend prediction from the<br />

measurement itself. Errors induced my motion and<br />

rotation are examined and corrected in the same way.<br />

In the end the elaborated corrections are applied<br />

flight tests that were undertaken during the course of<br />

this investigation.<br />

Project Objectives<br />

The Main Objectives are:<br />

- comparison of four similar sensors<br />

- statistical analysis of the universe<br />

- generation of a calibration curve<br />

- evaluation of the functioning of the calibration curve<br />

- conduction of flight tests to verify sensor data<br />

Project Conclusion<br />

In conclusion one can say that in the course of this<br />

investigation findings were made that did not match<br />

the desired outcome. Nevertheless the work done<br />

was not in vain. The results found exclude the<br />

Sentio32 sensor for use in the exact determination of<br />

aircraft position and attitude during flight and<br />

especially during spin. This is a valuable result since it<br />

indicates that another sensor has to be selected and<br />

installed before continuing with the inflight<br />

measurements of spin characteristics.

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