Electromagnetic-method-prospected primary-field loose-coupling reception device and method
A receiving device and electromagnetic method technology, applied in the field of electromagnetic method exploration, can solve problems such as strong mutual inductance, difficult resolution, and large changes in mutual inductance
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Embodiment 1
[0150] Embodiment 1, applied to the time-domain electromagnetic method, is carried out in the following order:
[0151] according to Figure 7 As shown, the central point O is selected on the plane, and the transmitting coil 2 is designed to be a 20-turn plane spiral coil, and each coil is approximately a circle; the radius of the innermost coil is 400mm, the radius of the outermost coil is 460mm, and the line width is 2.5mm. The distance between them is 0.5mm;
[0152] Design each sub-receiving coil as a 300-turn helical coil, and each turn of the coil is approximately a circle; the radius of the innermost coil is 100.5mm, the radius of the outermost coil is 120.5mm, the line width is 0.5mm, and the distance between lines is 0.5.
[0153] 2. Calculate the magnetic flux ψ passing through the sub-receiving coil m under the action of the primary field m1 (m=1, 2, 3, ... 7)
[0154]
[0155] Get: ψ m1 ≈1.5149×10 -9 i(t)(Wb)
[0156] 3. Start the transmitter, send as Fi...
Embodiment 2
[0164] Embodiment 2, applied to the frequency domain electromagnetic method, is carried out according to the following sequential steps;
[0165] 1, adopt the sending coil of embodiment 1 design, receiving coil group, get by the 2nd step of embodiment 1
[0166] ψ m1 ≈1.5149×10 -9 i(t) (Wb)
[0167] 2. Start the transmitter, send such as Figure 11 The sinusoidal current shown in the Figure 11 Middle: the horizontal axis is time t, each division is 0.02ms; the vertical axis is current, each division is 1A;
[0168] The signal is the sending current in Example 2. The frequency of the sending current is 10000 Hz. The sending current is measured by a current sensor. The conversion ratio of the current sensor is 100 mV / A, so the peak value of the sending current is 5.8 A. The sinusoidal current expression can be approximated: i(t)=5.5×cos(20000πt)(A);
[0169] 3. Calculate the primary field induced voltage of the inner receiving coil
[0170]
[0171] have to:
[0...
Embodiment 3
[0176] Embodiment 3, applied to the time-domain electromagnetic method, is carried out in the following order:
[0177] 1. Design of sending coil and receiving coil:
[0178] according to Figure 14 As shown, the central point O is selected on the plane, and the transmitting coil 2 is designed to be a 20-turn square solenoid; the side length of the square is 300mm, the line width is 2mm, and the distance between lines is 3mm;
[0179] The sub-receiving coil is designed as a 300-turn square solenoid; the side length of the square is 110mm, the line width is 2mm, and the distance between lines is 1.8mm;
[0180] 2. Calculate the magnetic flux ψ passing through the inner receiving coil 1 under the action of the primary field m1 :
[0181]
[0182] Get: ψ m1 ≈2.3149×10 -9 i(t) (Wb)
[0183] Among them: l 1 : The side length of each turn of the sub-receiving coil;
[0184] x: the x-coordinate of a point on the i-th coil plane of the sub-receiving coil;
[0185] y: the y...
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