The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1928 - English periodicals |
From inside the book
Results 1-5 of 99
Page vii
... Plane Boundary Distributions Mr. L R. G. Treloar on the Intensity Distribution of the General and Characteristic X - Radiation from Molybdenum Dr. L. F. Richardson on the Amount of Uniformly - diffused Light that will go in Series ...
... Plane Boundary Distributions Mr. L R. G. Treloar on the Intensity Distribution of the General and Characteristic X - Radiation from Molybdenum Dr. L. F. Richardson on the Amount of Uniformly - diffused Light that will go in Series ...
Page 102
... plane called the z plane to a portion of a uniform rectangular field in a plane called the x plane . If x and y are the coordinates of a point 102 Messrs . R. T. Coe and H. W. Taylor : Some Problems in.
... plane called the z plane to a portion of a uniform rectangular field in a plane called the x plane . If x and y are the coordinates of a point 102 Messrs . R. T. Coe and H. W. Taylor : Some Problems in.
Page 103
... plane . Points in the various planes are represented by the complex quantities ? = § + jn , 51 = §1 + jn1 , etc. Since the only figures considered have straight line boundaries , the Schwarz transformation theorem can be employed to ...
... plane . Points in the various planes are represented by the complex quantities ? = § + jn , 51 = §1 + jn1 , etc. Since the only figures considered have straight line boundaries , the Schwarz transformation theorem can be employed to ...
Page 104
... Plane S = ∞ S = ∞ S == k1 3/2 S = YK , S = - S = k 2 S = Χ 9 SPlane 77 * Plane S - 1 S = -x , S = -00 S = ∞0 S = YK1 S = 1 Flux - distribution in an air - gap uniformly slotted on one side . amount j2 as increases through the value ...
... Plane S = ∞ S = ∞ S == k1 3/2 S = YK , S = - S = k 2 S = Χ 9 SPlane 77 * Plane S - 1 S = -x , S = -00 S = ∞0 S = YK1 S = 1 Flux - distribution in an air - gap uniformly slotted on one side . amount j2 as increases through the value ...
Page 107
... planes we now turn to that between the plane and x plane , the latter representing a uniform field . Since both the potential difference and amount of flux associated with the problem figure are finite , the upper half of the plane is ...
... planes we now turn to that between the plane and x plane , the latter representing a uniform field . Since both the potential difference and amount of flux associated with the problem figure are finite , the upper half of the plane is ...
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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