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| DSH 201A
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- b, n6 x( i/ C; ?" h+ H% a) K7 N7 S | Characteristics of D.C. electric circuits for verifying normal operation and making and breaking cap ...' v. M" ~+ O& \. b3 F
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) b+ @0 ]0 [# Q1 r: J: r | Generality
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4 u1 k. g$ o' B: }6 jTo 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:; N: E" d& w) G, B! m- g/ ~
- Voltage drop
! x& ]- d+ H0 B5 L9 ?7 bThe maximum voltage drop which should not be exceeded, when passing from noload5 B6 r, p: L- T5 A
to load condition, is 5% of the rated voltage.; R& `3 M7 J: o8 @* r
- Voltage ripple value
. N; O3 |( X, G D9 O/ dThe supply voltage ripple, at no-load condition, should not exceed 5%.4 a- |1 {4 P4 o. [. c; D" y
NOTES:
* t% \; K3 a' P1 r5 q( D$ z- 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.3 R, G* {1 R. \2 D
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.3 W* P1 N/ T2 l5 D. n' e4 y" c
- The limitation of the ripple, which occurs, in practise, in rectifying converters, may be obtained choosing appropriately a rectifying bridge.0 D! I5 o. l: J2 C
- The use of a three-phase rectifying bridge, which gives a theoretical ripple of about 4,2%, complies with this recommendation.
. s7 }+ `% \5 x$ V- Recovery voltage, O, a, Q4 Q; F: \" o$ B u9 e" U6 R
Test circuit, where:
T4 U( ?$ t5 l! F; ~- E is the supply voltage at no-load condition;& H9 s7 O6 F/ m; k& V# _
- Li is equivalent to the different self-inductances of the supply as well as the stray inductances of the rest of the test circuit;* D$ L: H" b# q; `
- Cp is the stray capacitance of the circuit;! Y% ~0 \4 s( I
- Rp is the parallel damping resistance.& v, L4 H7 b2 p0 N* B7 X* ^
Neglecting the parallel damping resistor, Rp, the parameters Li and Cp should be adjusted so as to obtain:' t6 }$ g2 V9 @* W
- Li = 2·10-3 H ± 25%, and
4 X# ]$ P# _. z: @3 c- Cp = 50 mF ± 25%.8 H ]/ Q& |5 r( N* ^% c
NOTE - Adopting the above mentioned parameters, all CTL Laboratories will get approximately
2 b8 J A2 ^8 h8 s; Z D5 S- the same time constant T = Li / Ri = 2·10-3 / Ri;
, G0 o" T3 M2 y; ^( u- the same oscillatory frequency fo = 1 / 2· (Li Cp)1/2 500 Hz.
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