Grid-connected inverter parallel system circulating current restraining method under imbalance condition of inductance
A circulation suppression and balance condition technology, applied in the field of circulation suppression, can solve problems such as large circulation
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specific Embodiment approach 1
[0046] Specific implementation mode one: refer to figure 1 and image 3 Describe this embodiment in detail. In the method for suppressing the circulation of grid-connected inverter parallel system under the condition of unbalanced inductance described in this embodiment, the grid-connected inverter in the grid-connected inverter parallel system is a common DC bus, AC The side is directly connected in parallel, and the parallel system is controlled by the PI method. Aiming at the above-mentioned circulation suppression method for the parallel system of grid-connected inverters, this method is for one inverter of the grid-connected inverter in the parallel system of two inverters. The circulation of the device is controlled, which specifically includes the following steps:
[0047] Step 1: To the zero-sequence current i of the second inverter 2 z2 Sampling is performed, and then step 2 is performed;
[0048] Step 2: Using the zero-sequence current PI controller to control the...
specific Embodiment approach 2
[0054] Specific embodiment 2: This embodiment is to further explain the circulating current suppression method of grid-connected inverter parallel system under the condition of inductance imbalance described in specific embodiment 1. In this embodiment, in step 1, the second inverter 2 The zero sequence current i z2 for:
[0055] i z 2 = i a 2 + i b 2 + i c 2 3 - - - ( 1 )
[0056] where i k2 (k=a, b, c) are the a-phase, b-phase and c-phase currents of the second inverter 2 respectively.
specific Embodiment approach 3
[0057] Specific embodiment 3: This embodiment is to further explain the circulating current suppression method of grid-connected inverter parallel system under the condition of inductance imbalance described in specific embodiment 1. In this embodiment, the Δd mentioned in step 3 12 for:
[0058] Δd 12 =(d 21 -d 11 )-(d 22 -d 12 ) (2)
[0059] where d 11 is the duty cycle of the first non-zero vector of the first inverter, d 21 is the duty cycle of the second non-zero vector of the first inverter, d 12 is the duty cycle of the first non-zero vector of the second inverter 2, d 22 is the duty cycle of the second non-zero vector of the second inverter 2.
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