Waves, Lines, Radiation, And Frequency

#1Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7531

pi = 6li = kli, (7)

#2General Lectures on Electrical EngineeringLecture 6: Higher Harmonics Of The Generator Wave- line 3222

If m == number of phases, the higher harmonics : 2m - i

#3General Lectures on Electrical EngineeringLecture 7: High Frequency Oscillations And Surges- line 3624

2g3 QQQ = ^ seconds; the frequency 587 cycles, and if this

#4Radiation, Light and IlluminationLecture 9: Measurement Of Light And Radiation- line 8720

L -T- S = x2 -T- 7/2, where x and y are the two distances of the

#5Theoretical Elements of Electrical EngineeringTheory Section 1: Magnetism and Electric Current- line 822

line carrying 7 amperes of current, if Id = 0.82 cm. is the diam-

#6Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1458

1. Since x’i’ has relative to xi the velocity f, it is, for a;’ = 0:ax - bt = 0,

#7Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 2202

be V = Vi -{- V2 = 1.8c, or greater than the velocity of

#8Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 2249

velocity V2, it is Xi = v^h, and substituting this in the

#9General Lectures on Electrical EngineeringLecture 7: High Frequency Oscillations And Surges- line 3633

as for instance, lOO feet = ^230 ~ 52^ miles wave length,

#10General Lectures on Electrical EngineeringLecture 7: High Frequency Oscillations And Surges- line 3728

i5ioo + ^ + n^ + Wo = ^ -ond, so giving a

#11Radiation, Light and IlluminationLecture 1: Nature And Different Forms Of Radiation- line 859

lw = 60 microcentimeters,* that is, 60 X 10~8 cm. (or about

#12Radiation, Light and IlluminationLecture 1: Nature And Different Forms Of Radiation- line 860

^<y^<5-<y in.) and since the speed is S = 3 X 1010 cm. the frequency

#13Radiation, Light and IlluminationLecture 1: Nature And Different Forms Of Radiation- line 978

motions of very high speed, S = 3 X 1010 cm. per sec. in a hypo-

#14Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1674

medium TF, only the distance CK = - 2 GH, and the wave front

#15Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1690

and a2 = angle of refraction, that is, the angle between the out-

#16Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1703

FH + DL = S, - S3; (2)

#17Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1750

S = -L= , (5)

#18Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1785

Vl = d*-, (9)

#19Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1790

Since for most media the permeability /JL = 1, for all except

#20Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2827

Z0 = 51.1, bluish green for very low intensity, curve (a).

#21Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2828

Z0 = 53.7, yellowish green for medium intensity, curve (b).

#22Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 3976

Pr = kA (TV - ?V), (1)

#23Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 3981

k = 5 X 1(T12; (2)

#24Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 3997

Pr = kA (T, - T2) (TV + T*T2 + 7\7y + 7y);

#25Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4000

Pr = 4 kAT* (T, - T), (3)

#26Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4016

stationary air A^ reaches values as high as fct = 25 X 10~12 to

#27Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4027

Pr = kATf; (4)

#28Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4186

P- f °°P (lw)dlw = Mr-1;

#29Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4205

lmT =- = 0.284;

#30Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4674

k = bk0 = (1 - a) fcc,

#31Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4703

Curve II, for albedo a = 0.3, has the height 1 - a = 0.7 times

#32Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4715

constant 1 - a = 0.4 times that of the black body. Colored

#33Radiation, Light and IlluminationLecture 7: Flames As Illuminants- line 6953

a = 4, corresponding to a non-luminous flame, as observed. In

#34Radiation, Light and IlluminationLecture 7: Flames As Illuminants- line 6956

atoms is a = 2.8, or b = 30, corresponding to a luminous non-

#35Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7199

intersect in a point which lies at I = - 0.125 cm. = - 0.05 in.

#36Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7201

consists of a part, e0 = 30 (for the magnetite arc), which is con-

#37Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7237

constant value of current: el = k^ (I + 0.12), as function of

#38Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7241

ei = TT1-’ (1

#39Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7295

which is equation (1), and herefrom, since e = e0 + eir follows

#40Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7311

k = 31 for magnetite (123 in inch measure),

#41Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7336

e0 = 36 volts, but I, = - 0.8 cm. = - 0.33 in.; that is, a

#42Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7419

part. With a series resistance of r = 10 ohms, a 1.8-cm. mag-

#43Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7535

e = e0 + ev

#44Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7547

e0 = 13 volts ; k = -y-

#45Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7735

L = k’li, (9)

#46Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7739

ei = p] (10)

#47Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7743

e=e0 + ^ (11)

#48Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7764

L = - (pVi - ejVi), (13)

#49Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7808

i = 4: e = 75 volts, and I + l^ = 0.73 in., or about f-in. arc

#50Radiation, Light and IlluminationLecture 9: Measurement Of Light And Radiation- line 9232

10 deg. gives d = - - TT. This usually is done graphically.

#51Theoretical Elements of Electrical EngineeringTheory Section 3: Generation of E.m.f.- line 1214

50%Q = 8.33 rev. per sec. Thus the frequency is/ = 4 X 8.33

#52Theoretical Elements of Electrical EngineeringTheory Section 4: Power and Effective Values- line 1420

#o = E X \/2 = 273 volts per line;

#53Theory and Calculation of Alternating Current PhenomenaChapter 1: Introduction- line 1231

the period of the wave, or N = 1 / T is the frequency or

#54Theory and Calculation of Electric CircuitsChapter 3: Magnetism- line 5812

Below ff = 3, p is not a straight line, but curved, due to the in-

#55Theory and Calculation of Electric CircuitsChapter 3: Magnetism- line 5814

straight-line law is reached at the point Ci, at ff = 3, and the re-

#56Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1657

Let then Sl = speed of propagation in medium A, S2 = speed of

#57Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 4179

where a = 5 for normal temperature radiation or black body

#58Radiation, Light and IlluminationLecture 8: Arc Lamps And Arc Lighting- line 7368

point, at zero arc length, or e0’ = 28 volts. This looks as if, of

#59General Lectures on Electrical EngineeringLecture 7: High Frequency Oscillations And Surges- line 3679

- ’ - = 25,000. If now somewhere in the middle of this

#60Radiation, Light and IlluminationLecture 4: Chemical And Physical Effects Of Radiation- line 3701

and these free atoms then join existing molecules: 0 + 02 = 03,

#61Theory and Calculation of Alternating Current PhenomenaChapter 5: Symbouc Mbthod- line 3039

29. If /= / +ji’ is a sine wave of alternating current,

#62Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 1600

appear as L = 0, that is, would vanish, while at a velocity

#63Four Lectures on Relativity and SpaceLecture 2: Conclusions From The Relativity Theory- line 2200

with the same velocity, but in opposite direction, V2 = 0.9c.

#64Radiation, Light and IlluminationLecture 1: Nature And Different Forms Of Radiation- line 1303

Zero point chosen at c = 128 cycles per second.

#65Radiation, Light and IlluminationLecture 1: Nature And Different Forms Of Radiation- line 1304

Speed of radiation S = 3 X lu10 cm.

#66Radiation, Light and IlluminationLecture 2: Relation Of Bodies To Radiation- line 1694

FDH = a, and LHD = a2 ;

#67Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2464

1 to 2, but the change of sensation in the first case, log 1000 = 3,

#68Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2726

Wave length lw = 67 60.5 57.5 50.5 47 . 43 x 10~fl

#69Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2729

tensity … i0 = 0.06 0.0056 0.0029 0.00017 0.00012 0.00012

#70Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2733

power po = 10,000 1000 100 1 2 20

#71Radiation, Light and IlluminationLecture 3: Physiological Effects Of Radiation- line 2787

I = 45.0

#72Radiation, Light and IlluminationLecture 5: Temperature Radiation- line 3972

tor and T2 = absolute temperature of the surrounding objects

Waves, Lines, Radiation, And Frequency

Why This Family Matters

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