Page 242 - Rashid, Power Electronics Handbook
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14 Inverters 231
eliminate an odd N ÿ 1(N ÿ 1 ¼ 3; 5; 7; ...) number of where V o1 is the fundamental rms ac output voltage, I is the
o
harmonics are given by rms load current, f is an arbitrary inductive load power factor,
and I is the dc link current that can be further simpli®ed to
i
N
P k 2 ÿ p^ v =v i
o1
ÿ ðÿ1Þ cosðna Þ¼ V
k
k¼1 4 I ¼ o1 I cosðfÞ ð14:14Þ
o
i
V i
N
P k 1
ÿ ðÿ1Þ cosðna Þ¼ for n ¼ 3; 5; ... ; 2N ÿ 1
k
k¼1 2 14.2.2 Full-Bridge VSI
ð14:11Þ
Figure 14.8 shows the power topology of a full-bridge VSI.
where a ; a ; ... ; a N should satisfy a < a < < a < This inverter is similar to the half-bridge inverter; however, a
2
N
1
1
2
p=2. second leg provides the neutral point to the load. As expected,
both switches S and S (or S and S ) cannot be on
To implement the SHE modulating technique, the modu- 1þ 1ÿ 2þ 2ÿ
simultaneously because a short circuit across the dc link
lator should generate the gating pattern according to the
voltage source v would be produced. There are four de®ned
angles as shown in Fig. 14.7. This task is usually performed i
(states 1, 2, 3, and 4) and one unde®ned (state 5) switch states
by digital systems that normally store the angles in look-up
as shown in Table 14.2.
tables.
The unde®ned condition should be avoided so as to be
always capable of de®ning the ac output voltage. In order to
14.2.1.4 DC Link Current
avoid the short circuit across the dc bus and the unde®ned ac
The split capacitors are considered part of the inverter and
output voltage condition, the modulating technique should
therefore an instantaneous power balance cannot be consid-
ensure that either the top or the bottom switch of each leg is
ered due to the storage energy components (C and C ).
þ ÿ on at any instant. It can be observed that the ac output voltage
However, if a lossless inverter is assumed, the average power
can take values up to the dc link value v , which is twice that
i
absorbed in one period by the load must be equal to the
obtained with half-bridge VSI topologies.
average power supplied by the dc source. Thus, we can write
Several modulating techniques have been developed that are
applicable to full-bridge VSIs. Among them are the PWM
ð ð
T T
v ðtÞ i ðtÞ dt ¼ v ðtÞ i ðtÞ dt ð14:12Þ (bipolar and unipolar) techniques.
o
i
i
o
0 0
where T is the period of the ac output voltage. For an
inductive load and a relatively high switching frequency, the
load current i is nearly sinusoidal and therefore only the
o
fundamental component of the ac output voltage provides
power to the load. On the other hand, if the dc link voltage
remains constant v ðtÞ¼ V , Eq. (14.12) can be simpli®ed to
i
i
ð T 1 ð T p p
i ðtÞ dt ¼ 2V sinðotÞ 2I sinðot ÿ fÞ dt ¼ I
i o1 o i
0 V i 0
ð14:13Þ FIGURE 14.8 Single-phase full-bridge VSI.
TABLE 14.2 Switch states for a full-bridge single-phase VSI
State State # v aN v bN v o Components Conducting
S 1þ and S 2ÿ are on and S 1ÿ and S 2þ are off 1 v i =2 ÿv i =2 v i S 1þ and S 2ÿ if i o > 0
if i o < 0
D 1þ and D 2ÿ
S 1ÿ and S 2þ are on and S 1þ and S 2ÿ are off 2 ÿv i =2 v i =2 ÿv i D 1ÿ and D 2þ if i o > 0
if i o < 0
S 1ÿ and S 2þ
S 1þ and S 2þ are on and S 1ÿ and S 2ÿ are off 3 v i =2 v i =2 0 S 1þ and D 2þ if i o > 0
if i o < 0
D 1þ and S 2þ
s 1ÿ and S 2ÿ are on and S 1þ and S 2þ are off 4 ÿv i =2 ÿv i =2 0 D 1ÿ and S 2ÿ if i o > 0
if i o < 0
S 1ÿ and D 2ÿ
S 1ÿ , S 2ÿ , S 1þ , and S 2þ are all off 5 ÿv i =2 v i =2 ÿv i D 1ÿ and D 2þ if i o > 0
v i =2 ÿv i =2 v i D 1þ and D 2ÿ if i o < 0