Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Formula Map

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300

Formula and equation candidates.

136

Strong formula candidates.

66

Reviewable relation candidates.

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Formula Families

Family	Candidates
Transients, Oscillation, And Damping	300

Highest-Priority Candidates

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