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| DSH 201A
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% ^9 Q/ J. B4 z- Y; J | Characteristics of D.C. electric circuits for verifying normal operation and making and breaking cap ...
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4 O4 V7 D% |9 W8 n0 u | Generality" _! l- v' V0 |6 L5 I0 d
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8 _1 I0 S. _$ j2 g" kTo reach an acceptable test reproducibility, when verifying normal operation and making and breaking capacity, it is recommended that the test circuit has the following characteristics:1 L& K: X% n; v" V% L
- Voltage drop
" K& w6 l$ B/ {: _The maximum voltage drop which should not be exceeded, when passing from noload
7 O7 q: r7 B2 s# a+ ?0 a2 yto load condition, is 5% of the rated voltage.+ ~4 S( n; @8 O0 V7 m
- Voltage ripple value: Y6 U" r% Z% ?. I0 h J
The supply voltage ripple, at no-load condition, should not exceed 5%.
5 j9 A6 {" J: f* N: z4 @NOTES:
- u/ [/ S* x9 F$ a, U3 n( A- Percentage ripple is given by r% = Vac/Vdc x 100, where Vac is the RMS value of the superimposed a.c. voltage and Vdc is the d.c. voltage.# X, [. T; _* U/ G! G- P% O" J1 x: N
A simple way to evaluate the ripple is to use an oscilloscope, whose input is selected in a.c. for the measurement of Vac and in d.c. for the measurement of VDU.% u9 Y# F L7 T/ p" i
- The limitation of the ripple, which occurs, in practise, in rectifying converters, may be obtained choosing appropriately a rectifying bridge.* Y! u% f$ U, Q9 b: q6 U c t [
- The use of a three-phase rectifying bridge, which gives a theoretical ripple of about 4,2%, complies with this recommendation.
( ~% i& ^- l L1 k2 n- Recovery voltage* M9 c6 z9 v2 V( s8 k
Test circuit, where:* L+ j7 L) `+ C% m+ Z
- E is the supply voltage at no-load condition;$ t& Z& W3 d2 Y6 K. d. G
- Li is equivalent to the different self-inductances of the supply as well as the stray inductances of the rest of the test circuit;
! C3 Y; P/ J! J6 b) y5 L- Cp is the stray capacitance of the circuit;
8 a+ Y; v- o7 j& l- Rp is the parallel damping resistance.1 H$ O2 J2 n7 J' b
Neglecting the parallel damping resistor, Rp, the parameters Li and Cp should be adjusted so as to obtain:
) u. }4 W* i6 F( G' k* P# K- Li = 2·10-3 H ± 25%, and
# O9 ?2 e$ [% w* f% D# H# D- Cp = 50 mF ± 25%.
1 V- b$ {. O. K- n8 ]! ]4 C4 cNOTE - Adopting the above mentioned parameters, all CTL Laboratories will get approximately# w+ @4 P" m/ @) A- Z4 X
- the same time constant T = Li / Ri = 2·10-3 / Ri;
5 h9 K+ d; X5 [" o0 y; W2 Z( A- the same oscillatory frequency fo = 1 / 2· (Li Cp)1/2 500 Hz.
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