The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1928 - English periodicals |
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Page 34
... becomes blocked and more open alternately . The wave - front of pressure intensity ( and therefore of velocity potential ) will travel backwards along the stream toward the source as long as the slit wall in its alternations gives freer ...
... becomes blocked and more open alternately . The wave - front of pressure intensity ( and therefore of velocity potential ) will travel backwards along the stream toward the source as long as the slit wall in its alternations gives freer ...
Page 44
... becomes , as he has shown . ( Wellenmechanik ' ) , p . 514 , d2P ST ? dq2 + ( E。- 2π2vo2 q2 ) P = 0. . h2 · ( 49 ) If , then , we set α = 8π2E0 h2 b = 16π1vo2 h2 the equation becomes . d2P day dq2 + ( a − bq2 ) P = 0 = dq2 + ( a ...
... becomes , as he has shown . ( Wellenmechanik ' ) , p . 514 , d2P ST ? dq2 + ( E。- 2π2vo2 q2 ) P = 0. . h2 · ( 49 ) If , then , we set α = 8π2E0 h2 b = 16π1vo2 h2 the equation becomes . d2P day dq2 + ( a − bq2 ) P = 0 = dq2 + ( a ...
Page 47
... becomes d P = x + dq ( log Y ) . Dealing , then , with ( 60 ) instead of ( 51 ) , we know that x = Aq • • • ( 62 ) is a solution . This should at least lead to the result ( 54 ) as well as ( 57 ) . Introducing ( 62 ) in ( 60 ) gives ...
... becomes d P = x + dq ( log Y ) . Dealing , then , with ( 60 ) instead of ( 51 ) , we know that x = Aq • • • ( 62 ) is a solution . This should at least lead to the result ( 54 ) as well as ( 57 ) . Introducing ( 62 ) in ( 60 ) gives ...
Page 49
... becomes more and more closed as one blows harder and harder . That is , the Planck constant h is split up according to the formula h = hoh1 . Introducing the above factors into the differential equation of wave - motion results in the ...
... becomes more and more closed as one blows harder and harder . That is , the Planck constant h is split up according to the formula h = hoh1 . Introducing the above factors into the differential equation of wave - motion results in the ...
Page 82
... becomes , by one of several possible processes , doubly ionized ; i . e . , it lacks one K - electron and one M - electron . First , let us say , the vacant M shell is filled by an electron dropping from an optical orbit for which ...
... becomes , by one of several possible processes , doubly ionized ; i . e . , it lacks one K - electron and one M - electron . First , let us say , the vacant M shell is filled by an electron dropping from an optical orbit for which ...
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absorption aluminium apparatus approximately atomic number atomic weight axis B₁ Balmer series bands beam calculated calorimeter carbon cathode cent chamber coefficient coil colour corresponding cosh crystal curve d₁ deflexion determined diamagnetic diffusion discharge doublet effect electric electrolytes electrometer electrons electroscope energy equation excited experimental experiments fibre filter finite flux-density forbidden line formula fraction frequency function galvanometer gases given gives glass heat hydrogen increase indicated intensity ionization ionization chamber ions K₁ layer liquid magnetic maximum measurements mercury metal method molecules nitrogen observed obtained oscillator particles Phil photo-electric Phys plane plate potassium potential pressure problem Proc radiation radon ratio reflexion resistance salts satellites Schwarz theorem sensitivity shows sinh slit slot sn² solution spectrum surface Table temperature theory tube values vapour variation velocity viscosity voltage volts wave-length width X-ray y-rays zero