Consider a long thin conducting wire carrying a uniform current I. A particle having mass "m" and charge "q" is released at a distance "a" from the wire with a speed v0 along the direction of current in the wire. The particle gets attracted to the wire due to magnetic force. The particle turns round when it is at distance x from the wire. The value of x is [ 0 is vacuum permeability]
- a [1 - mv02q 0 I ]
- ae- 4 m v0q 0 I
- a [1 - mv0q 0 I ]
- a2
Answer
(2) ae- 4 m v0q 0 I
Solution
Take the wire along the z-axis (current along +z) and the particle in the x-z plane at distance r.
Field at the particle: B = 0 I2 r, along +y
Force F = q v B with v = vr i + vz k
Fz = qvrB = q drdt 0 I2 r
m dvz = q 0 I2 drr
Integrating from r = a (vz = v0) to r = x:
m(vz - v0) = q 0 I2 xa
Magnetic force does no work, the speed always remains v0.
At the turning point vr = 0, so |vz| = v0; the velocity has reversed, vz = -v0
-2mv0 = q 0 I2 xa
xa = - 4 m v0q 0 I
x = ae- 4 m v0q 0 I
Answer: (2)