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| Characteristics of D.C. electric circuits for verifying normal operation and making and breaking cap ...- l* ~9 D8 L! [# \, k; t
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+ k' s# F L! v. m/ n | Generality/ ]! L5 c! n2 ]" V
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& ^6 B% S" w# YTo 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:
; U- Y6 i# y( r7 q- ^8 i- Voltage drop
1 \& @. d6 G8 Y8 i: t2 d" mThe maximum voltage drop which should not be exceeded, when passing from noload) f+ V8 Z% c0 r% v; C- Z
to load condition, is 5% of the rated voltage.
) I. N! ?6 Q# ?/ N6 [# w- Voltage ripple value) P; P; g. {3 A6 f1 [9 r- S, z9 M
The supply voltage ripple, at no-load condition, should not exceed 5%.$ S! h+ ~ u+ \3 q; [& o
NOTES:
! \) G7 Y! t/ h+ ^( g9 b8 q- 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." {1 W p- X+ R& G: u8 d5 Y
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.. k5 k& `4 g9 N1 E3 o( \# U
- The limitation of the ripple, which occurs, in practise, in rectifying converters, may be obtained choosing appropriately a rectifying bridge.
0 V/ ?# w& F) [ p" N2 ]- The use of a three-phase rectifying bridge, which gives a theoretical ripple of about 4,2%, complies with this recommendation.5 [' B2 j& \0 o7 M1 Z1 I
- Recovery voltage+ ~3 R3 d4 Y+ ^0 ^$ U
Test circuit, where:
0 M) m/ o# b4 l, D( @- E is the supply voltage at no-load condition;
! V; c1 e# h# J- Li is equivalent to the different self-inductances of the supply as well as the stray inductances of the rest of the test circuit;
4 h: u6 O9 @# m$ m1 w, D- Cp is the stray capacitance of the circuit;
Q- \+ j4 G: \8 j$ l- Rp is the parallel damping resistance.2 J) R/ ]% z8 _- N
Neglecting the parallel damping resistor, Rp, the parameters Li and Cp should be adjusted so as to obtain:
+ m7 X% d$ P* z; G2 s1 h* K- Li = 2·10-3 H ± 25%, and! i3 S# z( W0 p( t# ~# Z- a
- Cp = 50 mF ± 25%.
: I# g& _1 B3 I. gNOTE - Adopting the above mentioned parameters, all CTL Laboratories will get approximately
+ N* f' v; E; x/ ~- the same time constant T = Li / Ri = 2·10-3 / Ri;, k7 B- A3 v# \" b- a. [
- the same oscillatory frequency fo = 1 / 2· (Li Cp)1/2 500 Hz.' o* B) w% f2 K' h
% ]6 k' ~% |3 a1 _7 T9 r1 H$ b: }& P& v2 G3 _# R% f7 j! I
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