eberhard pulz karl-heinz jäckel, oliver bronkalla

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Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

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Page 1: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Eberhard PulzKarl-Heinz Jäckel, Oliver Bronkalla

Page 2: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

1. Introduction

2. Serson’s Method

3. Cs-He-Magnetometer

4. Measuring Method

5. Coil System and Switching Technique

6. Theoretical Estimations and Limits

7. Design of Coil System

8. Installation of the Instrument

9. Results

10. Conclusion

1. Introduction

2. Serson’s Method

3. Cs-He-Magnetometer

4. Measuring Method

5. Coil System and Switching Technique

6. Theoretical Estimations and Limits

7. Design of Coil System

8. Installation of the Instrument

9. Results

10. Conclusion

Page 3: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Serson‘s Method

20

22

222

2220

222

222

2/

4

FFFA

A

FFST

TSF

ATSF

ATSF

A - additional field strengthFo - magnetic field strength without an additional fieldF+/- magnetic field strength with an additional fieldS – auxiliary quantityT – magnetic field strength at desired direction

F 0

T - A

A

T

F_

S

F+

Page 4: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Cs-He-Magnetometer

Cs - Lamp

Cs- Sensor

Cs-He- Sensor

Page 5: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

He Conversations Formula

0236888.28

frequencyF

Page 6: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Measuring Sequence for Each Second

180 msec

0 200 400 600 800 1000 timemsecfrequency counter in current switching

operation 180 msec

C+ E- F C- E+

True North

Bias field

Top view

Page 7: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Measurement Arrangement

Magnetometer Electronics

Switching Unit

Current source

Frequency Counter

GPS10MHz

Clock

LINUXComputer

SensorCoils

Page 8: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Estimation of Errors

Additional field strength for a given magnetometer noise about 0,005nT rmsand a desired noise in the components of 0,01nT rms

additional field strength of about 5000nT

Effect of tilting of the vertical axis of the bias coilfor ±1’tilting, we got for X= ±13nT

Effect of tilting the azimuth angle between the additional Field and the magnetic meridian

for ±1’tilting, we got for Y= ±5,5nT ΔX= ±3E-03

Page 9: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 10: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 11: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

.g

North South

MirrorLaser

PSD (20x20mm2)(Position Sensitive Diode)

Top viewTop view

E

a

mE

2tan

9

g = 1’ is about 5mm at PSD

a

Coil system

Page 12: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 13: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 14: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 15: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 16: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

s=2.1•10-2

s=8•10-3

s=1.9•10-2

Page 17: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 18: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 19: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 20: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 21: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla
Page 22: Eberhard Pulz Karl-Heinz Jäckel, Oliver Bronkalla

Conclusions

Cs-He magnetometer absolute accuracy 0.1 nTsum of noise at NGK < 5 pT rms @ 180 msec

Orthogonal coil system: suspended, turnable, LASER controlled

Realtime (GPS) LINUX-controlled system

Result: 1 sec mean values for all components

Reducing the number of manually absolute measurements to some / year

Thank you for your attention