Theoretical Elements of Electrical Engineering Formula Map

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.

111

Reviewable relation candidates.

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Formula Families

Family	Candidates
Inductance, Capacity, And Stored Energy	120
General Equation Candidates	87
Power, Energy, Work, And Efficiency	38
Symbolic AC And Complex Quantities	30
Magnetism, Hysteresis, And Core Loss	11
Waves, Lines, Radiation, And Frequency	8
Impedance, Reactance, And Admittance	3
Engineering Mathematics Foundations	2
Apparatus, Machines, And Power Systems	1

Highest-Priority Candidates

Candidate	Family	OCR/PDF text	Routes
`theoretical-elements-electrical-engineering-eq-candidate-0102` strong-formula-candidate	symbolic-ac	e = 2 7r/n $sin r the instantaneous generated e.m.f.</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-03/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-03/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0132</code><br/><small>strong-formula-candidate</small></td><td>symbolic-ac</td><td><code>If an alternating current i = I0 sin 6 passes through a resist-</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-04/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-04/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0138</code><br/><small>strong-formula-candidate</small></td><td>symbolic-ac</td><td><code>e.m.f., e = EQ sin 6.</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-04/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-04/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0049</code><br/><small>strong-formula-candidate</small></td><td>symbolic-ac</td><td><code>cos r = - - - - = 0.4</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-01/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-01/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0061</code><br/><small>strong-formula-candidate</small></td><td>general-equation-candidates</td><td><code>2$ = 0.4 X 105 / log, TT^ = 0.4 X 105 X 4.70 I = 0.188 X 106 7,	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0071` strong-formula-candidate	symbolic-ac	`iron is /z4 = 280 at B4 = 2850. Thus the field intensity/ H = - j`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0105` strong-formula-candidate	symbolic-ac	e = 2 irfn $sin 2 IT} (t - ti)</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-03/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-03/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0106</code><br/><small>strong-formula-candidate</small></td><td>symbolic-ac</td><td><code>or, e = 2-jrfn& sin (6 - 0i),</code></td><td><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/source-texts/theoretical-elements-electrical-engineering/section-03/">source</a><br/><a href="/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/theoretical-elements-electrical-engineering/section-03/">workbench</a></td></tr> <tr><td><code>theoretical-elements-electrical-engineering-eq-candidate-0108</code><br/><small>strong-formula-candidate</small></td><td>general-equation-candidates</td><td><code>E = 4/n$ > = generated e.m.f. ($ in megalines, / in	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0133` strong-formula-candidate	symbolic-ac	`i*r = 702r sin2 0 = ^r C1 ~ cos 2 0),`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0168` strong-formula-candidate	symbolic-ac	`e = E0 sin (0 - 0i) = 273 sin (0 - 0i) ;`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0170` strong-formula-candidate	symbolic-ac	`e = 273 sin 210 (t - h).`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0197` strong-formula-candidate	symbolic-ac	`e = - -j-. L 108 absolute units`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0244` strong-formula-candidate	inductance-capacity	`e-o.296 1 = 0.5, - 0.296 Mog e = log 0.5, t =`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0284` strong-formula-candidate	symbolic-ac	`34. An alternating current i = IQ sin 2irft or i - I0 sin 0`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0288` strong-formula-candidate	symbolic-ac	`i = /0 sin 2 IT/ (t - t’),`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0291` strong-formula-candidate	symbolic-ac	`i = IQ sin 6 passes through a circuit of resistance r and induc-`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0297` strong-formula-candidate	symbolic-ac	`2 irft = /o sin 0) of effective value`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0298` strong-formula-candidate	symbolic-ac	`e’2 = - xI0 cos 2 irft = - xIQ cos 6,`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0300` strong-formula-candidate	symbolic-ac	`e’z = - xIQ cos 0,`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0290` strong-formula-candidate	symbolic-ac	`If such a sine wave of alternating current i = IQ sin 2 irft or`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0053` strong-formula-candidate	waves-radiation	`line carrying 7 amperes of current, if Id = 0.82 cm. is the diam-`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0243` strong-formula-candidate	inductance-capacity	`(a) M strength: i = ~, hence (1 - €-°-29«0 = 0.5.`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0246` strong-formula-candidate	symbolic-ac	`(b) %0 strength: i = 0.9 *0j hence (1 - e-°-2960 = 0.9, and`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0277` strong-formula-candidate	inductance-capacity	`(d) If i = 0 at * = 0.0005, then`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0280` strong-formula-candidate	inductance-capacity	`(e) If t = - I = - 90 at t = 0.001, then`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0047` strong-formula-candidate	symbolic-ac	`sin T = 0.2 mlo sin r, the torque of the current is`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0050` strong-formula-candidate	symbolic-ac	`In equilibrium, 0.2 mlQ sin r = 0.4 mlQ cos r, or tan r = 2,`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0083` strong-formula-candidate	general-equation-candidates	`ated e.m.f. is E = 12.5 volts.`	source workbench
`theoretical-elements-electrical-engineering-eq-candidate-0100` strong-formula-candidate	general-equation-candidates	`E = 4 fn& is the average generated e.m.f.,`	source workbench