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Theory and Calculation of Transient Electric Phenomena and Oscillations Formula Map

Review layer: these are OCR/PDF-text formula candidates. Promote only after scan verification, mathematical transcription, and notation review.

300

Formula and equation candidates.

93

Strong formula candidates.

76

Reviewable relation candidates.

FamilyCandidates
Transients, Oscillation, And Damping300
CandidateFamilyOCR/PDF textRoutes
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0272
strong-formula-candidate
transients-oscillationAt the moment 0 = 0, let the e.m.f. e = E cos (0 - 00) besource
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0276
strong-formula-candidate
transients-oscillationSince e = E cos (0 - 00) = impressed e.m.f.,source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0296
strong-formula-candidate
transients-oscillationi = -z | cos (I? - 00- 0J- i~x° cos (00 + OJ j (9)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0137
strong-formula-candidate
transients-oscillationi = I cos (d - 45°),source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0193
strong-formula-candidate
transients-oscillatione = ir (l - -J; (10)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0196
strong-formula-candidate
transients-oscillationt = 0, i = iv log cii = 0, c = - ,source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0236
strong-formula-candidate
transients-oscillationt = 26.8 log 17.9log(31.252.5- 17.9 log (31.25 - 2.5) + 79.6 (37)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0237
strong-formula-candidate
transients-oscillationt = 26.8 log e - 17.9 log (31.25 - 0.125 e) - 0.8. (38)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0258
strong-formula-candidate
transients-oscillationt = 0.04 log e - 0.01333 log (600 - e) - 0.08. (44)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0263
strong-formula-candidate
transients-oscillationt = 0.0274 log e - 0.00073 log (876 - e) - 0.1075, (45)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0278
strong-formula-candidate
transients-oscillationi = 7 cos (6 - d) + A£~a°, (2)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0285
strong-formula-candidate
transients-oscillationE cos 00 - Ir cos d - Ix sin d = 0,source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0286
strong-formula-candidate
transients-oscillationE sin 00 - Ir sin d + Ix cos d = 0,source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0292
strong-formula-candidate
transients-oscillationi = - cos (0 - 00 - 0X) + As x , (7)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0300
strong-formula-candidate
transients-oscillationi =— cos (d - 60 - ^)-cos (00 + 0,)- e* . (10)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0153
strong-formula-candidate
transients-oscillationLet e0 = 125 volts = impressed e.m.f. of the circuit, andsource
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0184
strong-formula-candidate
transients-oscillatione.m.f., and the constants of the circuit then are: e0 = 250source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0146
strong-formula-candidate
transients-oscillationHence, eQ = ir + L - > (1)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0148
strong-formula-candidate
transients-oscillationhence, i = il + (i0 - t\) e ’ , (3)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0165
strong-formula-candidate
transients-oscillationLet, in a continuous-current shunt motor, e0 = 250 volts =source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0271
strong-formula-candidate
transients-oscillationit is usually employed, the reactance x = 2 nfL, where / = fre-source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0136
strong-formula-candidate
transients-oscillatione = E cos 0,source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0192
strong-formula-candidate
transients-oscillationand since full speed S and full flux <I>0 generate an e.m.f. e0 =source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0275
strong-formula-candidate
transients-oscillationor, by substituting 6 = 2 nft, x = 2 nfL, the e.m.f. consumedsource
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0072
strong-formula-candidate
transients-oscillationP = ie (1)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0073
strong-formula-candidate
transients-oscillation<E> = Li = the intensity of the electromagnetic field. (2)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0074
strong-formula-candidate
transients-oscillationMf = Ce = the intensity of the electrostatic field. (3)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0075
strong-formula-candidate
transients-oscillationet = ri, (4)source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0077
strong-formula-candidate
transients-oscillationor, by equation (2) : <J> = Li by definition, thus :source
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0078
strong-formula-candidate
transients-oscillation- = L-,and: P’ = Lt-, (7)source
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