Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Formula Map
Formula Map
Section titled “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.
136
Strong formula candidates.
66
Reviewable relation candidates.
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Formula Families
Section titled “Formula Families”| Family | Candidates |
|---|---|
| Transients, Oscillation, And Damping | 300 |
Highest-Priority Candidates
Section titled “Highest-Priority Candidates”| Candidate | Family | OCR/PDF text | Routes |
|---|---|---|---|
electric-discharges-waves-impulses-1914-eq-candidate-0240strong-formula-candidate | transients-oscillation | e = 2;oCe-”’ sin (0 =F co - 7) j | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0293strong-formula-candidate | transients-oscillation | i = e~ ”’ J ai cos </) cos co + 6i sin cf) cos co + Ci cos 0 sin co | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0018strong-formula-candidate | transients-oscillation | f = j (13) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0029strong-formula-candidate | transients-oscillation | K = j^; (21) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0135strong-formula-candidate | transients-oscillation | (S!,J = 20,000 lines per cm^. * | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0159strong-formula-candidate | transients-oscillation | T = 2.92 - { 9.21 log’^ , ,\ . + .921 log’^ i ’ ^ ^ | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0162strong-formula-candidate | transients-oscillation | division with log^^e = .4343. | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0163strong-formula-candidate | transients-oscillation | t = im^log’H- .507. | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0179strong-formula-candidate | transients-oscillation | ^l = ^o cos 7 = initial transient current. (14) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0180strong-formula-candidate | transients-oscillation | e = eo sin (0 - 7), (15) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0181strong-formula-candidate | transients-oscillation | ei = - 60 sin 7 = initial value of transient voltage. (16) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0189strong-formula-candidate | transients-oscillation | i = ^o cos (0 - t) = io cos y cos 4> + io sin y sin 0 | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0190strong-formula-candidate | transients-oscillation | i = ii cos 2/0^1 sin-, (21) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0199strong-formula-candidate | transients-oscillation | I = e~^^ < Zi cos 2/0^1 sm - | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0215strong-formula-candidate | transients-oscillation | { = e-3^U40cos0.2^ -80 sin 0.2^ J | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0216strong-formula-candidate | transients-oscillation | e = e- ^‘S 2000 cos 0.2 ^ + 3500 sin 0 | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0217strong-formula-candidate | transients-oscillation | i’ = 140 cos 0.2 t - 80 sin 0.2 1, | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0218strong-formula-candidate | transients-oscillation | e’ = 2000 cos 0.2 i + 3500 sin 0.2 1. | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0223strong-formula-candidate | transients-oscillation | ii = Iq cos (0 - 7) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0228strong-formula-candidate | transients-oscillation | e = eoe~ ^^ sin (0 - 7) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0231strong-formula-candidate | transients-oscillation | e’ = -eo sin 7 | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0239strong-formula-candidate | transients-oscillation | i = ce-”’ COS ((/) =F CO - 7) ) . | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0267strong-formula-candidate | transients-oscillation | lo = vto = -.J (32) | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0294strong-formula-candidate | transients-oscillation | e = e- w« 5 di cos <f) cos co + W sin </> cos co + c/ cos </> sin co | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0055strong-formula-candidate | transients-oscillation | zero of time, ^o = 0, and equations (5) then assume the simpler | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0140strong-formula-candidate | transients-oscillation | where Q = a plus the reluctance of the air gap. Equation (1), | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0198strong-formula-candidate | transients-oscillation | This is correct only if g = 0, that is, the conductance, which rep- | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0232strong-formula-candidate | transients-oscillation | tuting {t =F ^i) instead of t into the equations (11), where ^i is the | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0272strong-formula-candidate | transients-oscillation | length Zo = 4 k, and therefore the period ^0 = co^o = 4 aoh, that | source workbench |
electric-discharges-waves-impulses-1914-eq-candidate-0274strong-formula-candidate | transients-oscillation | the frequencies (2 k - l)/o, where k = 1,2,3 .. . | source workbench |