Controllable source electromagnetic simulation wave number sequence optimization method based on elimination strategy
A technology of electromagnetic simulation and optimization method, which is applied in design optimization/simulation, complex mathematical operation, special data processing application, etc. It can solve the problem that the optimal wave number selection method cannot be proposed and cannot meet the calculation accuracy requirements of ocean controllable source electromagnetic forward modeling. and other problems, to achieve the effect of improving speed and computing efficiency, fast computing speed and high efficiency
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Embodiment 1
[0028] The invention provides a controllable source electromagnetic simulation wavenumber sequence optimization method based on elimination strategy. The method adjusts the relative position of each node of the wavenumber sequence by solving the problem of optimizing the electromagnetic field response of the wavenumber simulation and the minimum value of the target data, based on redundancy The elimination strategy of wave number gradually eliminates redundant wave numbers by optimizing wave number algorithm 1 and optimizing wave number algorithm 2, and finally obtains an optimized wave number sequence. Therefore, the optimized wavenumber sequence composed of a small number of wavenumber nodes is used to obtain simulation results with high precision, which greatly improves the speed and efficiency of simulation calculation.
[0029] see figure 1 , a wavenumber sequence optimization method for controllable source electromagnetic simulation based on elimination strategy, which ...
Embodiment 2
[0061] As we all know, the case of resistivity anisotropy is more complicated than that of resistivity isotropy. When ocean controllable source forward modeling performs wave number domain and time domain conversion, the case of resistivity anisotropy needs a relatively denser wave number sequence to obtain Same Fourier transform calculation accuracy as resistivity isotropy. In order to illustrate the effectiveness and adaptability of this algorithm, a more complex case of resistivity anisotropy will be selected for discussion in the optimal wavenumber calculation example.
[0062] see figure 2 , is a schematic diagram of the structure of the one-dimensional resistivity anisotropy model. In order to compare the accuracy of different wavenumber sequences, based on figure 2 The model shown is taken as an example to carry out forward calculation with different wavenumber sequences. It is assumed that the seawater layer with a depth of 300m is isotropic in resistivity, and its...
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