General Equation Candidates

#1Theoretical Elements of Electrical EngineeringTheory Section 1: Magnetism and Electric Current- line 858

2 $ = 0.4 X 105 / log, TT^ = 0.4 X 105 X 4.70 I = 0.188 X 106 7,

#2Theoretical Elements of Electrical EngineeringTheory Section 3: Generation of E.m.f.- line 1174

E = 4/n $> = generated e.m.f. ($ in megalines, / in

#3Theory and Calculation of Electric CircuitsChapter 2: Electric Conduction. Gas And Vapor- line 4701

Pi = 6i i = c -y/i {I + 8)

#4Theory and Calculation of Electric CircuitsChapter 3: Magnetism- line 5817

Pi = 0.102 + 0.059 H (7)

#5Theory and Calculation of Electric CircuitsChapter 3: Magnetism- line 6167

of soft material of reluctivity pi (ferrite) and g = 1 - p of hard

#6Theory and Calculation of Electric CircuitsChapter 3: Magnetism- line 6211

p = 0.80 : pi = 0.082 + 0.0477 H,

#7Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 8198

log w = log 7} + n log B, (19)

#8Theory and Calculation of Electric CircuitsChapter 6: Magnetism- line 11334

PI = ^ \ . ^ gram-cm. (22)

#9Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 2259

If then vx = 0.9c and V2 = 0.9c, v = 1.8c/1.81 = 0.9945c;

#10General Lectures on Electrical EngineeringLecture 5: Long Distance Transmission- line 3023

the resistance, or 10 ohms. The current therefore - = ~r =

#11Theory and Calculation of Alternating Current PhenomenaChapter 1: Introduction- line 1134

1. Ohm’s law: i = -, where r, the resistance, is a constant

#12Theory and Calculation of Alternating Current PhenomenaChapter 1: Introduction- line 1408

posed, hence, i = 2ir NCe the current passing into the con-

#13Theory and Calculation of Alternating Current PhenomenaChapter 2: Chapter II- line 1825

B^ the sine varies from to OB = 1. Hence the average

#14Theory and Calculation of Alternating Current PhenomenaChapter 9: Kbsistanci: And Kbactance Of Transmission Iine8- line 7327

67. If tf = 1, that is, if the voltage at the receiver cir-

#15Theory and Calculation of Alternating Current PhenomenaChapter 9: Kbsistanci: And Kbactance Of Transmission Iine8- line 7332

If dr = 1 when ^ = 0, ^ =

#16Theory and Calculation of Alternating Current PhenomenaChapter 9: Kbsistanci: And Kbactance Of Transmission Iine8- line 7421

If ^^ = 2 r^, orjr^ = r^ V3, the maximum output, P =

#17Theory and Calculation of Electric ApparatusChapter 1: Speed Control Of Induction Motors- line 2613

jni’iea-cil secondary resistance: ■> where ri = 0.1 in the

#18Theory and Calculation of Electric CircuitsChapter 2: Electric Conduction. Gas And Vapor- line 4740

It seems as if the terminal drop, a = 36 volts with carbon, con-

#19Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 8032

rj = 0.824 X 10-3 fQj. ^i^Q medium range, where n = 1.6

#20Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 8048

n = 1.6 for the medium range, where ij = 0.0824 X 10-‘

#21Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 8049

Ml = 2 for the low range, where in = 0.0457 X 10”*

#22Theory and Calculation of Electric CircuitsChapter 5: Magnetism- line 9101

^^ lower intrinsic saturation value. Thus, if S = 21 X 10’ is

#23Theoretical Elements of Electrical EngineeringTheory Section 2: Magnetism and E.m.f.- line 991

ated e.m.f. is E = 12.5 volts.

#24Theoretical Elements of Electrical EngineeringTheory Section 3: Generation of E.m.f.- line 1097

E = 4 fn& is the average generated e.m.f.,

#25Theoretical Elements of Electrical EngineeringTheory Section 3: Generation of E.m.f.- line 1196

generated e.m.f. is 0.151 H volts. Since this is = 0.028 volt,

#26Theoretical Elements of Electrical EngineeringTheory Section 3: Generation of E.m.f.- line 1217

The generated e.m.f. is E = 550 volts, thus by the formula of

#27Theory and Calculation of Alternating Current PhenomenaChapter 4: Graphic Representation- line 2244

mary coil, an E.M.F. Ex = I0x0 is required, 90° ahead of

#28Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 7990

from log B = 3; B = 1000, to log B = 4; B = 10,000, with slope

#29Theory and Calculation of Electric CircuitsChapter 4: Magnetism- line 7991

1.6006, and for low densities, up to log B = 2.6; B = 400, with

#30Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1272

c = ~7E=^ = 3 X IQio cm.,

#31Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1388

value - that is, assume x = 0, t = 0, x’ = 0, t’ = 0,

#32Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1495

x’ = a{x - vt) 1

#33Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1526

i’ = ^= or i = ^= (2)

#34Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1577

from the train^ - is U = X2’ - Xi ; in track coordinates -

#35Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1611

between the same events is T = to - ti. However, by (2) :

#36Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1680

the time i\\ that is, the length of the train is L = X\- X2.

#37Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1762

s^ = (X2 - x^y + {u -hy = (xo’ - xi’Y + {k - uY =s’^

#38Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1772

{X2 - xi)2 - c\U -hy = (x./ - Xi’Y - c\t,’ - h’Y, (5)

#39Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1814

w = ct (6)

#40Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1882

*S^ = (0:2 - Xi)^ - {w-i - WiY =

#41Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1894

u = jet’, (10)

#42Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1904

x’ = -r==l or: X = ~. (11)

#43Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1997

S’- = (x, - x,y + (i/2 - yiY + (22 - z,y + {U2 - u^y =

#44Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 2182

light- by (3) and (4), L = 0 and T = oo. That is, on

#45Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2426

F = HP (1)

#46Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2441

F=KQ, (2)

#47Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2449

F = gN, (3)

#48Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2458

F = CR, (4)

#49Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2471

W = Mvy2, (5)

#50Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2478

a = F/M, (6)

#51Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2690

per cent, and the acceleration thus is a = 0.1^ = 2.2 miles

#52Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2800

Fc = Mvyi (9)

#53Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 2818

Fo = -Mvyi (11)

#54Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3061

CO = CO 2 - COi. (13)

#55Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3067

C02 = V^/C

#56Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3077

CO = (^2 - Vi)/C. (15)

#57Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3082

Vi - Vi = gt; (16)

#58Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3087

co= gt/c (17)

#59Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3189

C = ird. (19)

#60Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3469

2/K = 1.08 X 20” cm.

#61Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3476

P = 3 X 10-”.

#62Four Lectures on Relativity and SpaceLecture 3: Gravitation And The Gravitational Fleld- line 3487

V = 2w^R’^

#63Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 3774

conditions: C = ird, > 7r(iand<7rd.

#64Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4501

/vi = 1/R, (3)

#65Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4549

R = VR1R2 = -^ (6)

#66Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4554

I = 27rR (7)

#67Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4564

A = 4x7^2 (8)

#68Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4568

V = 4.ir’R’/S ’ (9)

#69Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4583

R = l/VK. (10)

#70Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4594

z = 0; (12)

#71Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 4605

R = l/VK. (14)

#72Four Lectures on Relativity and SpaceLecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational Field- line 5013

P4 = r - I 1 1 ’ (4)

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