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AN1889 bảng dữ liệu(PDF) 20 Page - STMicroelectronics

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Giải thích chi tiết về linh kiện  The need to choose a high value of the fly-back voltage
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Current transformer core selection
AN1889
20/33
In Figure 10 the driving circuit as been modeled with the equivalent schematic diagram of
the transformer with its secondary closed with a voltage generator. In fact, looking at
Figure 9 we must note that during on time, the base of ESBT can be seen as a forward
biased diode, to this we have to add the voltage drop on both diode D and resistor RB in
series with the base of the ESBT to complete the secondary side load model. With these
premises in a first order of analysis, the secondary side can be simply modeled as a voltage
source given by:
Equation 27
At primary side both primary inductance and magnetization inductance have been reported.
Considering that only the IP fraction of the total collector current will be transferred to the
secondary, the magnetization current has to be firstly as low as possible, secondly, its value
must been taken into account for the proper calculation of transformer turn ratio. The
magnetization voltage drop (that is the voltage at the primary of the current transformer) can
be now easily calculate:
Equation 28
The magnetization current for the two cores under analysis will be:
Equation 29
and
Equation 30
Being the IPmax=0.9 A in steady state, the N67 core with 2 turns at primary side must
obviously be excluded, unless increasing the number of turns, but this would lead to fill all
the available window area and consequently to the necessity of choosing a bigger core size.
Figure 9.
ESBT current transformer
driver
Figure 10.
ESBT equivalent circuit
VS
V1
IC
V
s
V
BEon
V
D
V
RB
2.5V
≅
++
=
V
1
V
S
N
1T
N
2T
----------
•
2.5
1
5
---
0.5V
=
•
=
=
I
Mmax
V
1TONmax
L
TP
----------------------------
0.5
10.66
•
19.8
-----------------------------
0.27
=
=
=
For N30
I
Mmax
V
1TONmax
L
TP
----------------------------
0.5
10.66
•
4.28
-----------------------------
1.24
=
=
=
For N67



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