Difference between revisions of "6DOF Electromagnetic Tracker Construction HOWTO"

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* Frederick H. Raab, "Quasi-Static Magnetic-Field Technique for Determining Position and Orientation", IEEE Transactions on Geoscience and Remote Sensing, Vol. GE-19, No. 4, October 1981, pages 235-243.
 
* Frederick H. Raab, "Quasi-Static Magnetic-Field Technique for Determining Position and Orientation", IEEE Transactions on Geoscience and Remote Sensing, Vol. GE-19, No. 4, October 1981, pages 235-243.
  
[[File:Dry0097.c]]
+
* [[File:Dry0097.c]] is a simulator program containing an implementation of Raab's algorithm.
  
 
Much elaboration and extension is needed to give high accuracy with high convenience, but the above is the basic idea.
 
Much elaboration and extension is needed to give high accuracy with high convenience, but the above is the basic idea.

Revision as of 01:41, 29 June 2011

Home < 6DOF Electromagnetic Tracker Construction HOWTO

A basic 6DOF (six degrees of freedom) electromagnetic tracker contains the following parts:

  • Transmitter contains three colocated orthogonal coils.
  • Receiver contains three colocated orthogonal coils.
  • Driver electronics provides three sinewaves at distinct frequencies through three series-tuning capacitors to the three transmitter coils.
  • Operating frequencies are typically 30 Hz to 15000 Hz. 1000 Hz, 1300 Hz, and 1600 Hz are a good starting point. Higher frequencies give higher induced voltages, lower frequencies reduce error-causing eddy-current effects.
  • Data-acquisition electronics measures the currents in the three transmitter coils, and measures the voltages induced in the three receiver coils. The voltage preamps should have 2 nV/sqrt(Hz) or lower input noise. The ADC sampling rate must be high enough to capture the driver frequencies.
  • A six-ADC electronics can measure all the currents and voltages continually and simultaneously.
  • A four-ADC electronics can use one channel to measure the three currents periodically over time (The currents change slowly as the transmitter coils warm up.), and three channels to measure the three voltages continually and simultaneously.
  • A single-ADC electronics can measure the currents and voltages sequentially, but this gives poor dynamic performance due to inconsistent data sets.
  • Signal-processing software converts the current and voltage measurements into measurements of the HFluxPerI coupling from each transmitter coil to each receiver coil. This gives a 3x3 matrix HFluxPerIMeasured.
  • Each component of HFLuxPerIMeasured is the H flux through one receiver coil, divided by the current I in one transmitter coil. HFLuxPerIMeasured has units of meters, and is a geometrical property of the coils' sizes, shapes, number of turns, positions, and orientations.
  • Algorithm software converts HFluxPerIMeasured to estimated receiver position and orientation, using direct-solution algorithm in Raab's 1981 paper:
  • Frederick H. Raab, "Quasi-Static Magnetic-Field Technique for Determining Position and Orientation", IEEE Transactions on Geoscience and Remote Sensing, Vol. GE-19, No. 4, October 1981, pages 235-243.
  • File:Dry0097.c is a simulator program containing an implementation of Raab's algorithm.

Much elaboration and extension is needed to give high accuracy with high convenience, but the above is the basic idea.

Better than 1 millimeter P95 accuracy is achievable, as reported in this paper: C.A. Nafis, V. Jensen, L. Beauregard, P.T. Anderson, "Method for estimating dynamic EM tracking accuracy of Surgical Navigation tools", SPIE Medical Imaging Proceedings, 2006.