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Question: A straight conductor of mass m and carrying a current i is hinged at one end and placed in a plane p...

A straight conductor of mass m and carrying a current i is hinged at one end and placed in a plane perpendicular to the magnetic field B as shown in figure. At any moment if the conductor is let free, then the angular acceleration of the conductor will be (neglect gravity)–

A

3iB2 m\frac { 3 \mathrm { iB } } { 2 \mathrm {~m} }

B
C
D

3i2mB\frac { 3 \mathrm { i } } { 2 \mathrm { mB } }

Answer

3iB2 m\frac { 3 \mathrm { iB } } { 2 \mathrm {~m} }

Explanation

Solution

Torque dt = dF × rb = iBdr × r t = 0LiBrdr=iBL22\int _ { 0 } ^ { \mathrm { L } } \mathrm { iBrdr } = \frac { \mathrm { iBL } { } ^ { 2 } } { 2 }

a = τI\frac { \tau } { \mathrm { I } } = iBL22 mL23\frac { \mathrm { iBL } ^ { 2 } } { \frac { 2 \mathrm {~mL} ^ { 2 } } { 3 } } =