A Crack Distribution Detection Method Based on Rock Resistance Change
A technology of crack distribution and resistance change, which is applied in the direction of material analysis, measuring devices, and analysis materials through electromagnetic means, can solve the problems of large rock damage, complex experimental principles, and low detection efficiency, and achieve accurate crack distribution and matching The effect of simple equipment and low detection cost
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specific Embodiment 1
[0056] Specific embodiment 1, such as Figure 5 As shown, the temperature distribution diagram of the temperature spectrum of the disseminated metal rock, the internal metal particles of the disseminated metal rock are scattered throughout the volume, and each metal particle can have an excited polarization effect. Under the action of an external electric field, the induced polarization effect spreads throughout the interior of the rock. The induced polarization effect is reflected in the polarizability of the rock material and the dopant material inside the rock. The polarizability changes rapidly with time, and the nonlinear current density generated is also large. Specific Embodiment 1 When an external electric field is applied, the entire rock body will be in an excited polarization state, and induced polarization phenomena will occur at the rock body and rock cracks, generating polarization currents. Under the action of current, it can be seen from the law of thermodynam...
specific Embodiment 2
[0057] Specific embodiment 2, such as Image 6 As shown in the temperature distribution diagram of the temperature sensing map of non-mineral rocks, non-mineral rocks have a low degree of dispersion of metal particles inside, and the induced polarization effect will only occur on the wet part of the rock crack surface. Under the action of an external electric field, the induced polarization effect occurs at the rock cracks. The induced polarization effect reflects the polarizability at the rock crack, and the polarizability changes rapidly with time, resulting in a large nonlinear current density. Specific embodiment 2 When an external electric field is applied, the rock crack surface is in an excited polarization state, and a polarization current is generated. Under the action of current, it can be seen from the law of thermodynamics that part of the electric energy will be converted into heat. The greater the resistivity, the more heat will be generated when a large current...
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