A time-dependent variable resistance element (VR) has been added to NETWORK. An example analysis is shown in Fig. 1 for the model described in "Improvement of Power Supply Input Method"( with the addition of the variable resistor element.
The circuit represented in Fig. 1 is represented by the data in Table 1. Table 2 shows the input format for the time-dependent variable resistance element (VR). While a constant resistance value ($\Omega$) is entered for the resistance element ($R$), for the variable resistance element, the time variation of the resistance value is specified by a time variation identification number (TIME_ID). A variable resistance element ($VR$) can be given a step change in resistance as shown in Table 3. In this example, the resistance is zero from time 0 to 0.1 second, and 1 $k \Omega$ from 0.1 to 0.2 seconds. (This data is equivalent to the data for the switch used in the "Improvement of Power Supply Input Method".) Of course, a continuous resistance change can also be analyzed. The analysis results of this example are shown in Fig. 2 and are in good agreement with the analysis values calculated from the resistance and inductance of the coil.
Table 1. NETWORK Data
17.8.15 Variable resistance elements | ||||
---|---|---|---|---|
row | string | Name | Type | Content |
1 | 1 | VR | S | Title Represents time-dependent variable resistance. |
2 | ID | I | element identification number | |
3 | START | I | starting node number | |
4 | END | I | endpoint node number | |
5 | TIME_ID | I | Time-varying identification number (18). Resistance ($\Omega$) as a function of time. The time variation may be varied stepwise. |
Table 3. Example of resistance time variation data for variable resistance elements
・ input_var_resistor : Input condition file
・ pre_geom2D.neu : Mesh file
・ 2D_to_3D : 3D extension file
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