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(a) Deduce the expression for the torque acting on a dipole of dipole moment \vec{p} placed in a uniform electricfield \vec{E}. Depict the direction of the torque. Express it in the vector form.

(b) Show that the potential energy of a dipole making angle \theta with the direction of the field is given by u(\theta)=-\vec{p}.\vec{E}. Hence find out the amount of work done in rotating it from the position of unstable equilibrium to the stable equilibrium.

 

 

 

 
 
 
 
 

Answers (1)

(a)

 

Magnitude of Torque \tau =F\times 2a\; \sin \theta

                                       =qE\; 2a\; \sin \theta

                                       =PE\; \sin \theta

   Vector forme               =P\times E

The direction of the torque is perpendicular to P and E

(b) The amount of work done by external torque in rotating the dipole is stored as potential energy.

w=\int_{\theta _{o}}^{\theta }\tau d\; \theta =\int_{\theta _{o}}^{\theta _{1}}PE\; \sin \theta d\; \theta

     =PE\left ( \cos \theta _{o}-\cos \theta _{1} \right )

When \theta _{o}\rightarrow \frac{\pi }{2} and \theta _{1}\rightarrow \theta

w=-PE\cos \theta

For unstable equilibrium \theta _{o}=180^{o}

For stable equilibrium \theta _{1}=0^{o}

w=PE\left ( \cos \theta _{o}-\cos \theta _{1} \right )

     =PE\left ( \cos 180-\cos 0 \right )

      =-2PE

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Safeer PP

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