The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1928 - English periodicals |
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Page iv
... Equation ▽ ↓ = w in n - dimensional Euclidean Space 241 Mr. R. T. Lattey on the Influence of the Solvent on the Mobility of Electrolytic Ions . 258 Prof. R. W. Wood and Dr. E. Gaviola on the Factors governing the Appearance of the ...
... Equation ▽ ↓ = w in n - dimensional Euclidean Space 241 Mr. R. T. Lattey on the Influence of the Solvent on the Mobility of Electrolytic Ions . 258 Prof. R. W. Wood and Dr. E. Gaviola on the Factors governing the Appearance of the ...
Page 33
... Equation . By Prof. A. PRESS * . IN PART I. The Differential Equation of an Excitation Field . N a paper appearing in the Philosophical Magazine for Dec. 1927 , the writer likened the action of a radiating harmonic oscillator to that of ...
... Equation . By Prof. A. PRESS * . IN PART I. The Differential Equation of an Excitation Field . N a paper appearing in the Philosophical Magazine for Dec. 1927 , the writer likened the action of a radiating harmonic oscillator to that of ...
Page 35
... equation of the type Eo V = tho = Eo ho = / 1 ho ( + m2 2 · . max . ( 2 ) then the function solving equation ( 1 ) must be of the form P = P ( x ) . sin ( 2t ) . • • ( 3 ) This will enable a considerable simplification to be performed ...
... equation of the type Eo V = tho = Eo ho = / 1 ho ( + m2 2 · . max . ( 2 ) then the function solving equation ( 1 ) must be of the form P = P ( x ) . sin ( 2t ) . • • ( 3 ) This will enable a considerable simplification to be performed ...
Page 37
... equation -- q = − v2 ( k1 — k2i ) po † · P , we ( 15 b ) ( 16 ) That is to say , whenever radiation occurs the momentum p is not to be taken in time - phase with the velocity ġ of the displacement . The out - of - phase component ...
... equation -- q = − v2 ( k1 — k2i ) po † · P , we ( 15 b ) ( 16 ) That is to say , whenever radiation occurs the momentum p is not to be taken in time - phase with the velocity ġ of the displacement . The out - of - phase component ...
Page 38
... equations : where H = E + HT , Ho v pok , cos 2vt , Hv = E。= qu2po2ki . ( 20 ) The last of ( 20 ) , since it is ... equation ( 2 ) , which is fundamental in Quantum Theory , by the aid of ( 15 ) and ( 15 a ) we have for the velocity ...
... equations : where H = E + HT , Ho v pok , cos 2vt , Hv = E。= qu2po2ki . ( 20 ) The last of ( 20 ) , since it is ... equation ( 2 ) , which is fundamental in Quantum Theory , by the aid of ( 15 ) and ( 15 a ) we have for the velocity ...
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