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| DSH 201A
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| Characteristics of D.C. electric circuits for verifying normal operation and making and breaking cap ...( {3 `2 g2 L/ b' V1 q. I: ?, L
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| Generality+ }. k2 M! V& x3 {; b% f
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" ~$ O% I1 h! F& W) s' tTo 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 D/ ~ B! ^9 \9 \* r7 e2 N- Voltage drop
: Z' V M8 W, n7 a# j/ S' pThe maximum voltage drop which should not be exceeded, when passing from noload" m& l& f1 i& D3 a0 f" t1 G9 ^
to load condition, is 5% of the rated voltage.
. y H2 ` [! X- s& m8 \) A9 D- Voltage ripple value; Q5 }. s/ ~( x+ J
The supply voltage ripple, at no-load condition, should not exceed 5%.' z2 \) R: v: u" d5 m
NOTES:
7 ~$ N7 \8 H/ K4 g1 X% s- 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.
: R% }, t5 ?: C% J8 i9 D- vA 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! P) F6 o9 n2 l7 q# ]- The limitation of the ripple, which occurs, in practise, in rectifying converters, may be obtained choosing appropriately a rectifying bridge., P# t7 z s p% S- }
- The use of a three-phase rectifying bridge, which gives a theoretical ripple of about 4,2%, complies with this recommendation.4 U" ~8 n' b6 ]1 a
- Recovery voltage8 k$ @( C- |- }$ v. F/ Z4 \! z0 z: ]
Test circuit, where:
5 U# }/ d) D" E. y. k* i/ F& h! h- E is the supply voltage at no-load condition;: Z- W, q2 M) Q
- Li is equivalent to the different self-inductances of the supply as well as the stray inductances of the rest of the test circuit;: v& N1 v8 N* z k
- Cp is the stray capacitance of the circuit;
6 b4 n2 n2 p5 Q- Rp is the parallel damping resistance.
; O% j( i Q1 B% c/ ^# v2 L- lNeglecting the parallel damping resistor, Rp, the parameters Li and Cp should be adjusted so as to obtain:
' Q. V) L1 S# H1 q8 T, R& u- Li = 2·10-3 H ± 25%, and
6 z( |! Q1 g: M s- Cp = 50 mF ± 25%.' L4 } U$ I3 b
NOTE - Adopting the above mentioned parameters, all CTL Laboratories will get approximately
8 F, W$ S* U; {- the same time constant T = Li / Ri = 2·10-3 / Ri;
: H) }, G9 y+ P! C" [, g- the same oscillatory frequency fo = 1 / 2· (Li Cp)1/2 500 Hz.
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