different_power_gains
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| ===Overview output power within the gains=== | ===Overview output power within the gains=== | ||
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| + | ===Overview input power within the gains=== | ||
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| + | ====Simulation example==== | ||
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| + | As example, let us consider a very simple, purely resistive network, consisting of three resistors: | ||
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| + | //Figure 6: Simple, purely resistive, example network// | ||
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| + | We simulate the three gains in LT Spice with a DC voltage source of 12 V, as function of the generator resistance and the load resistance. | ||
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| + | //Figure 7: Schematics in LT Spice for the three gains, for the example network, with variable load and/or generator resistance {R}.// | ||
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| + | We first simulate the operating power gain $G_P$ as function of the load resistance. This gain is independent on the generator resistance. In the simulation, a generator resistance of 8.02773 ohm was chosen (see further), but this value doesn' | ||
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| + | The graph below (green) shows that a maximum of $G_P$ = 10.9% is reached for a load of 14.5 ohm. | ||
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| + | //Figure 8: Simulation results of the gains as function of varying generator or load resistance (logarithmic axis) for the given example.// | ||
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| + | Next, the available gain $G_A$ is simulated as function of varying generator resistance (this gains is independent on the value of the load). We find a maximum of 10.9% at a generator resistance of 8.0 ohm. | ||
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| + | Finally, the transducer gain $G_T$ is simulated, first for varying generator resistance, and next for varying load. The generator/ | ||
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| + | Links with One Relay Element. Wireless Power Transfer 2018, 5, 27–41. </ | ||
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