Theory and Calculation of Alternating Current Phenomena 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.
116
Strong formula candidates.
78
Reviewable relation candidates.
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Formula Families
Section titled “Formula Families”Highest-Priority Candidates
Section titled “Highest-Priority Candidates”| Candidate | Family | OCR/PDF text | Routes |
|---|---|---|---|
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0240strong-formula-candidate | symbolic-ac | is r - j (x -f x0} = r = .6, x + x0 = 0, and tan S>0 = 0 ; | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0001strong-formula-candidate | symbolic-ac | 1.) Ohm’s law : i = e j r, where r, the resistance, is a | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0131strong-formula-candidate | symbolic-ac | or, if E = e -\-je’ is the impressed E.M.F., and 7 = i ’ -\- ji’ | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0156strong-formula-candidate | apparatus-systems | E.M.F. of the generator OE°, where Z0 = r0 - jx0 = inter- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0281strong-formula-candidate | inductance-capacity | Then, if E0 = impressed E.M.F.,- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0032strong-formula-candidate | symbolic-ac | ty : i = 7i sin 2 TT N(t - A) + 7, sin 6 TT N (t - /3) | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0087strong-formula-candidate | symbolic-ac | E0 = V(^ cos w + Ir)2 -f- (E sin w + Ix)z. | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0113strong-formula-candidate | symbolic-ac | ffo = Vfr2 + S^2 + 20^ sin Wi, | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0123strong-formula-candidate | symbolic-ac | since y’2 = - 1, j = V- 1 ; | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0142strong-formula-candidate | symbolic-ac | - /V) , tan w0 = | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0219strong-formula-candidate | symbolic-ac | Z -jx0 = r-j(x +#e). | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0231strong-formula-candidate | symbolic-ac | circuit •- z= 1 Qj r = 1>0> x= 0 (Curve j) | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0244strong-formula-candidate | inductance-capacity | for the constant impressed E.M.F., E0 = 100 ; for the con- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0264strong-formula-candidate | symbolic-ac | &Q = ro JXoi ZQ = V f0 -j- Xo , | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0002strong-formula-candidate | power-energy | 2.) Joule’s law: P= izr, where P is the rate at which | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0003strong-formula-candidate | power-energy | 3.) The power equation : P0 = ei, where P0 is the | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0011strong-formula-candidate | inductance-capacity | circuits. Hence the inductance is L = $/ i = ;/2/(R. | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0159strong-formula-candidate | symbolic-ac | Let OIV Oly Of3 = three-phase currents in the receiver | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0164strong-formula-candidate | impedance-admittance | the term conductance, g = 1 / r. If, then, a number of con- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0170strong-formula-candidate | impedance-admittance | 1.) If r = QO , or x = oo , since in this case no current | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0173strong-formula-candidate | impedance-admittance | 2.) If r = 0, since in this case the current which passes | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0174strong-formula-candidate | impedance-admittance | 1.) If x = oo , or r = oo . | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0181strong-formula-candidate | impedance-admittance | a maximum for r = x, where g - 1 / 2 r is equal to the | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0224strong-formula-candidate | inductance-capacity | but E = E0,I= E0/z. If x0 < - 2 x, it raises, if x0 > - Zv, | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0225strong-formula-candidate | inductance-capacity | d.} If x = 0, that is, if the receiver circuit is non- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0255strong-formula-candidate | inductance-capacity | maximum for x0= +1.0, x = - 1.0, and r = 0, where | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0269strong-formula-candidate | inductance-capacity | since x = ~Vz2 - r2, if rr0 -f- x0 ~\/z2 - r2 is a maximum. | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0271strong-formula-candidate | inductance-capacity | f = rr0 + *0 Vs2 - r2 = maximum or minimum, if | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0018strong-formula-candidate | symbolic-ac | P0 = ei cos <£. | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0088strong-formula-candidate | impedance-admittance | E0> a resistance E.M.F., Er = fr, a reactance E.M.F., | source research review |