The conducting bar illustrated in Figure, moves on two frictionless, parallel rails in the presence of a uniform magnetic field directed into the page. The bar has mass m, and its length is l, The bar is given an initial velocity Vi to the right and is released at t=0. Using Newton’s law find and Proof the velocity of the bar as a function of time as a
The conducting bar illustrated in Figure, moves on two frictionless, parallel rails in the presence of a uniform magnetic field directed into the page. The bar has mass m, and its length is l, The bar is given an initial velocity Vi to the right and is released at t=0. Using Newton’s law find and Proof the velocity of the bar as a function of time as a
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The conducting bar illustrated in Figure, moves on two frictionless, parallel rails in the
presence of a uniform magnetic field directed into the page. The bar has mass m, and its length is
l, The bar is given an initial velocity Vi to the right and is released at t=0. Using Newton’s law
find and Proof the velocity of the bar as a function of time as a
Transcribed Image Text:a) In == -
B²1².
b) In = -(
- 27 = 1/2 (3
d) V
B²12
-)t
mR
t²-
B²12
mR
-B²1²t
mR
m2R
e) R = In - 2 (R
mR
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