Theory and Calculation of Electric Circuits 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.
102
Strong formula candidates.
99
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-electric-circuits-eq-candidate-0053strong-formula-candidate | general-equation-candidates | Pi = 6i i = c -y/i {I + 8) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0097strong-formula-candidate | general-equation-candidates | Pi = 0.102 + 0.059 H (7) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0105strong-formula-candidate | general-equation-candidates | of soft material of reluctivity pi (ferrite) and g = 1 - p of hard | source workbench |
theory-calculation-electric-circuits-eq-candidate-0106strong-formula-candidate | symbolic-ac | P2 = a2 + fT^H J | source workbench |
theory-calculation-electric-circuits-eq-candidate-0115strong-formula-candidate | general-equation-candidates | p = 0.80 : pi = 0.082 + 0.0477 H, | source workbench |
theory-calculation-electric-circuits-eq-candidate-0117strong-formula-candidate | symbolic-ac | inward bend of J?i below H = 2, are best shown (“Engineering | source workbench |
theory-calculation-electric-circuits-eq-candidate-0135strong-formula-candidate | symbolic-ac | J? = 1, may give any value of flux density between B = -4.6 | source workbench |
theory-calculation-electric-circuits-eq-candidate-0195strong-formula-candidate | general-equation-candidates | log w = log 7} + n log B, (19) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0244strong-formula-candidate | magnetism-hysteresis | Pi’actically non-magnetic, lowers the permeability to /x = 1.4. | source workbench |
theory-calculation-electric-circuits-eq-candidate-0283strong-formula-candidate | general-equation-candidates | PI = ^ \ . ^ gram-cm. (22) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0296strong-formula-candidate | symbolic-ac | FJ = j^ = -J- gram-cm. (29) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0065strong-formula-candidate | general-equation-candidates | It seems as if the terminal drop, a = 36 volts with carbon, con- | source workbench |
theory-calculation-electric-circuits-eq-candidate-0122strong-formula-candidate | symbolic-ac | Ai, at ff = - 1.5, J5 = -4, and then again reverse, we get a ris- | source workbench |
theory-calculation-electric-circuits-eq-candidate-0124strong-formula-candidate | magnetism-hysteresis | - 1.12, jB= - 1.0: the rising magnetization curve B ’” then passes | source workbench |
theory-calculation-electric-circuits-eq-candidate-0188strong-formula-candidate | general-equation-candidates | rj = 0.824 X 10-3 fQj. ^i^Q medium range, where n = 1.6 | source workbench |
theory-calculation-electric-circuits-eq-candidate-0190strong-formula-candidate | general-equation-candidates | n = 1.6 for the medium range, where ij = 0.0824 X 10-‘ | source workbench |
theory-calculation-electric-circuits-eq-candidate-0191strong-formula-candidate | general-equation-candidates | Ml = 2 for the low range, where in = 0.0457 X 10”* | source workbench |
theory-calculation-electric-circuits-eq-candidate-0230strong-formula-candidate | general-equation-candidates | ^^ lower intrinsic saturation value. Thus, if S = 21 X 10’ is | source workbench |
theory-calculation-electric-circuits-eq-candidate-0179strong-formula-candidate | general-equation-candidates | from log B = 3; B = 1000, to log B = 4; B = 10,000, with slope | source workbench |
theory-calculation-electric-circuits-eq-candidate-0180strong-formula-candidate | general-equation-candidates | 1.6006, and for low densities, up to log B = 2.6; B = 400, with | source workbench |
theory-calculation-electric-circuits-eq-candidate-0004strong-formula-candidate | general-equation-candidates | r = roT (1) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0013strong-formula-candidate | general-equation-candidates | i = ’-^^^ (2) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0045strong-formula-candidate | general-equation-candidates | r = roS-”^ (3) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0052strong-formula-candidate | general-equation-candidates | e = a + 7T- (4) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0054strong-formula-candidate | general-equation-candidates | ei = 7T- (5) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0064strong-formula-candidate | general-equation-candidates | by equation (4), and approaches for i = the value 6 = 28 volts. | source workbench |
theory-calculation-electric-circuits-eq-candidate-0076strong-formula-candidate | symbolic-ac | = a + 1.5 ^SL+J) (9) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0077strong-formula-candidate | general-equation-candidates | ei = d (10) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0086strong-formula-candidate | general-equation-candidates | M = a(S - B) (1) | source workbench |
theory-calculation-electric-circuits-eq-candidate-0088strong-formula-candidate | general-equation-candidates | for B = Oy equation (1) gives | source workbench |