Philosophical MagazineTaylor & Francis, 1913 - Physics |
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Page 581
... circuits at the time t as being equal to and K , E2 cos2 W2 · ω ] 2 t K , E2 sin2 W2 W1 2 t respectively . These expressions show that K , E2 , the whole of the energy in the system , passes from either circuit to the other and back to ...
... circuits at the time t as being equal to and K , E2 cos2 W2 · ω ] 2 t K , E2 sin2 W2 W1 2 t respectively . These expressions show that K , E2 , the whole of the energy in the system , passes from either circuit to the other and back to ...
Page 583
... circuit is equal to 4ab c2 K1E2 × sin'S ( say ) . If at the instant when S has all entered the radiating circuit for the first time the primary circuit be broken , then S will have to remain in the radiating circuit , which will now ...
... circuit is equal to 4ab c2 K1E2 × sin'S ( say ) . If at the instant when S has all entered the radiating circuit for the first time the primary circuit be broken , then S will have to remain in the radiating circuit , which will now ...
Page 768
... circuit . There are 4 circuit branches altogether , besides the steady exciting - current circuit of the stator ; the circuits of the rotor have been called R1 and R3 , those of the stator have been called R2 and R1 ; the latter circuit ...
... circuit . There are 4 circuit branches altogether , besides the steady exciting - current circuit of the stator ; the circuits of the rotor have been called R1 and R3 , those of the stator have been called R2 and R1 ; the latter circuit ...
Contents
SIXTH SERIES | 1 |
Dr N Bohr on the Theory of the Decrease of Velocity | 10 |
Dr S A Shorter on the Application of the Theory | 31 |
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