Radiation, Light and Illumination Formula Map

Formula Map

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300

Formula and equation candidates.

54

Strong formula candidates.

92

Reviewable relation candidates.

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Formula Families

Family	Candidates
Waves, Lines, Radiation, And Frequency	284
Symbolic AC And Complex Quantities	13
Magnetism, Hysteresis, And Core Loss	1
Transients, Oscillation, And Damping	1
Impedance, Reactance, And Admittance	1

Highest-Priority Candidates

Candidate	Family	OCR/PDF text	Routes
radiation-light-and-illumination-eq-candidate-0063 strong-formula-candidate	symbolic-ac	FH = DH sin a, and DL = DH sin av (1)	source workbench
radiation-light-and-illumination-eq-candidate-0198 strong-formula-candidate	symbolic-ac	cubic hyperbolas: e^i = kz2; or, el =- £j and since we find for	source workbench
radiation-light-and-illumination-eq-candidate-0235 strong-formula-candidate	waves-radiation	pi = 6li = kli, (7)	source workbench
radiation-light-and-illumination-eq-candidate-0300 strong-formula-candidate	symbolic-ac	fc1 = 2 TT / sin <t>dfa (3)	source workbench
radiation-light-and-illumination-eq-candidate-0281 strong-formula-candidate	waves-radiation	L -T- S = x2 -T- 7/2, where x and y are the two distances of the	source workbench
radiation-light-and-illumination-eq-candidate-0178 strong-formula-candidate	symbolic-ac	J in. or less diameter, even acetylene, a = 1, gives smokeless	source workbench
radiation-light-and-illumination-eq-candidate-0296 strong-formula-candidate	symbolic-ac	dA = 2 n sin	source workbench
radiation-light-and-illumination-eq-candidate-0014 strong-formula-candidate	waves-radiation	lw = 60 microcentimeters,* that is, 60 X 10~8 cm. (or about	source workbench
radiation-light-and-illumination-eq-candidate-0015 strong-formula-candidate	waves-radiation	^<y^<5-<y in.) and since the speed is S = 3 X 1010 cm. the frequency	source workbench
radiation-light-and-illumination-eq-candidate-0019 strong-formula-candidate	waves-radiation	motions of very high speed, S = 3 X 1010 cm. per sec. in a hypo-	source workbench
radiation-light-and-illumination-eq-candidate-0060 strong-formula-candidate	waves-radiation	medium TF, only the distance CK = - 2 GH, and the wave front	source workbench
radiation-light-and-illumination-eq-candidate-0061 strong-formula-candidate	waves-radiation	and a2 = angle of refraction, that is, the angle between the out-	source workbench
radiation-light-and-illumination-eq-candidate-0064 strong-formula-candidate	waves-radiation	FH + DL = S, - S3; (2)	source workbench
radiation-light-and-illumination-eq-candidate-0068 strong-formula-candidate	waves-radiation	S = -L= , (5)	source workbench
radiation-light-and-illumination-eq-candidate-0070 strong-formula-candidate	waves-radiation	Vl = d*-, (9)	source workbench
radiation-light-and-illumination-eq-candidate-0071 strong-formula-candidate	waves-radiation	Since for most media the permeability /JL = 1, for all except	source workbench
radiation-light-and-illumination-eq-candidate-0089 strong-formula-candidate	waves-radiation	Z0 = 51.1, bluish green for very low intensity, curve (a).	source workbench
radiation-light-and-illumination-eq-candidate-0090 strong-formula-candidate	waves-radiation	Z0 = 53.7, yellowish green for medium intensity, curve (b).	source workbench
radiation-light-and-illumination-eq-candidate-0104 strong-formula-candidate	waves-radiation	Pr = kA (TV - ?V), (1)	source workbench
radiation-light-and-illumination-eq-candidate-0105 strong-formula-candidate	waves-radiation	k = 5 X 1(T12; (2)	source workbench
radiation-light-and-illumination-eq-candidate-0106 strong-formula-candidate	waves-radiation	Pr = kA (T, - T2) (TV + T*T2 + 7\7y + 7y);	source workbench
radiation-light-and-illumination-eq-candidate-0107 strong-formula-candidate	waves-radiation	Pr = 4 kAT* (T, - T), (3)	source workbench
radiation-light-and-illumination-eq-candidate-0109 strong-formula-candidate	waves-radiation	stationary air A^ reaches values as high as fct = 25 X 10~12 to	source workbench
radiation-light-and-illumination-eq-candidate-0112 strong-formula-candidate	waves-radiation	Pr = kATf; (4)	source workbench
radiation-light-and-illumination-eq-candidate-0118 strong-formula-candidate	waves-radiation	P- f °°P (lw)dlw = Mr-1;	source workbench
radiation-light-and-illumination-eq-candidate-0120 strong-formula-candidate	waves-radiation	lmT =- = 0.284;	source workbench
radiation-light-and-illumination-eq-candidate-0127 strong-formula-candidate	waves-radiation	k = bk0 = (1 - a) fcc,	source workbench
radiation-light-and-illumination-eq-candidate-0130 strong-formula-candidate	waves-radiation	Curve II, for albedo a = 0.3, has the height 1 - a = 0.7 times	source workbench
radiation-light-and-illumination-eq-candidate-0132 strong-formula-candidate	waves-radiation	constant 1 - a = 0.4 times that of the black body. Colored	source workbench
radiation-light-and-illumination-eq-candidate-0186 strong-formula-candidate	waves-radiation	a = 4, corresponding to a non-luminous flame, as observed. In	source workbench