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TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative...

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Page 1: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 2: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 3: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 4: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 5: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 6: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 7: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 8: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 9: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 10: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 11: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 12: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 13: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 14: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 15: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 16: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 17: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 18: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 19: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 20: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 21: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 22: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 23: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 24: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 25: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 26: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 27: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 28: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 29: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

Page 30: TN12 - Geonics · vortex eddy currents is, in resistive ground, proportional to the time derivative of the primary magnetic field (and the transmitter current) and is thus an impulse

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