|
| DSH 201A
/ X# F- ^. ]" ?- i( q- ]; o( M0 K& J$ E" V4 c
| Characteristics of D.C. electric circuits for verifying normal operation and making and breaking cap ...$ B% }1 Q% U- N. y/ l0 p
| -
1 Q! I5 f; A9 E. w | Generality+ i5 @ U4 f/ f+ N( p# X# R6 }) t
|
. k- K. p0 G! h" J( ZTo 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:
7 A2 }7 W4 R; r( T7 i% h- Voltage drop
# l( @) q" n" e, K; t1 k# M$ q0 TThe maximum voltage drop which should not be exceeded, when passing from noload" _+ C ]# m: W1 Q
to load condition, is 5% of the rated voltage.
; n9 k& E( ~. j9 ~- Voltage ripple value
1 P, y5 @% O7 L8 P. R7 s" X/ MThe supply voltage ripple, at no-load condition, should not exceed 5%.
' m( ~, \9 h6 G/ X, wNOTES:
" i' b0 g" Z/ f4 u2 x. j$ G- 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.
- ]0 n- g) u S4 ^6 J: L- d# a( B AA 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.: i( r. ^. P0 R+ a% [ f
- The limitation of the ripple, which occurs, in practise, in rectifying converters, may be obtained choosing appropriately a rectifying bridge.
1 z% R, x1 i0 [' R- The use of a three-phase rectifying bridge, which gives a theoretical ripple of about 4,2%, complies with this recommendation." ~# K ?$ [4 }; D
- Recovery voltage
$ J* {& N# _2 i! r- `Test circuit, where:
& \$ u$ E, J! w- E is the supply voltage at no-load condition;* v" z7 b0 H* w/ P
- Li is equivalent to the different self-inductances of the supply as well as the stray inductances of the rest of the test circuit;
- J8 o( X9 ~+ O( O* @- L+ ~- Cp is the stray capacitance of the circuit;5 a) _) @: \; T0 |0 ~
- Rp is the parallel damping resistance.. _7 x9 `! V! j
Neglecting the parallel damping resistor, Rp, the parameters Li and Cp should be adjusted so as to obtain:" J2 B" w, z4 Z, i- k6 p/ y6 O
- Li = 2·10-3 H ± 25%, and! h$ J0 J" Z7 ]; Y( N" ]
- Cp = 50 mF ± 25%.& f/ p; t3 G! Q7 ?( J' v
NOTE - Adopting the above mentioned parameters, all CTL Laboratories will get approximately
; j5 B, e f1 z, k- the same time constant T = Li / Ri = 2·10-3 / Ri;$ c; g3 y1 U* ?7 U- |3 @
- the same oscillatory frequency fo = 1 / 2· (Li Cp)1/2 500 Hz.: { }) H) P) j' `7 @
$ a. T: e9 ^6 S- a6 H' P. j1 o$ A7 A" ~
3 P" I, [! c9 E; V% E, R R8 v" E; @9 u) T% f, r4 g( K
- T7 s# Y1 B5 n6 v; |( J6 U# m; V% i |
本帖子中包含更多资源
您需要 登录 才可以下载或查看,没有帐号?注册安规
x
|