Environmental Engineering Reference
In-Depth Information
i N
i L
1
ε
u v
u N
1
i c
0
K v
sC N
-
sL N
-
+
+
K i
Figure 11.4 Voltage-current control scheme for the neutral leg
both the voltage loop and the current loop, the two loop controllers can simply be designed as
proportional controllers K v and K i , respectively.
11.2.1 Design of the Current Controller K i
The objective of the current loop is to attenuate the effect of neutral current i N on i c as much
as possible, at least for those frequency components under consideration. For systems with
a fundamental frequency of 50 Hz, the highest frequency components under consideration
can be up to the 31st harmonics, i.e., 1550 Hz. Approximately, the corresponding angular
frequency is 10000 rad/s. As can be seen later, this is a crucial parameter for the performance
of the neutral point (the level of the shift
).
The transfer function from i N to i c in Figure 11.5(a) is
ε
sL N
sL N +
K i , of which the Bode plot
is shown in Figure 11.5(b). The corner angular frequency, called the inner loop (angular)
frequency, is
K i
ω i =
L N . As discussed in Section 11.1, the smaller the current i c , the smaller the
shift
ω i should be high
enough while considering the physical limit. 2 Hence, the current-loop control parameter is
ε
. In order to make i c as small as possible, the inner loop frequency
K i = ω i L N .
(11.4)
Here,
ω i is chosen as 10000 rad/s. Accordingly, the switching frequency f s is chosen as 10
kHz, which is larger than 3
4 times of 1550 Hz.
11.2.2 Design of the Voltage Controller K v
After the current loop is designed, the system shown in Figure 11.4 is equivalent to the one
shown in Figure 11.6, based on which the voltage controller K v can be designed.
The transfer function from i N to
ε
is
sL N
s 2 L N C N +
T ( s )
=
K v .
(11.5)
sK i C N +
2 As can be seen later in Figure 11.8, the larger the ω i , the higher the high frequency gain from i N to u N is required.
But this is usually limited by the low-pass filtering effect of the system.
 
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