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    Potential Energy Of A Dipole In An Electric Field - Practice Questions & MCQ

    Edited By admin | Updated on Sep 18, 2023 18:34 AM | #JEE Main

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    • 19 Questions around this concept.

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    Electric charges $q, q,-2 q$ are placed at the corners of an equilateral triangle ABC of side l. The magnitude of the electric dipole moment of the system is

    When an electric dipole $\vec{p}$ is placed in a uniform electric field $\vec{E}$ then at what angle between $\vec{p}$ and $\vec{E}$ the value of torque will be maximum

    A molecule with a dipole moment p is placed in an electric field of strength E. Initially the dipole is aligned parallel to the field. If the dipole is to be rotated to be anti-parallel to the field, the work required to be done by an external agency is

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    For stable equilibrium, the angle between dipole moment $\vec{p}$ and electric field $\vec{E}$ must be:

    If we place an electric dipole S in a uniform electric field W. The dipole has minimum potential energy when the angle between S and W in degrees will be

    Concepts Covered - 1

    Electric potential energy of an electric dipole

    When a dipole is kept in a uniform electric field. The net force experienced by the dipole is zero as shown in the below figure.

    I.e Fnet = 0

     

    But it will experience torque. And Net torque about the center of dipole is given as

    $\tau=Q E d \sin \theta$ or $\tau=P E \sin \theta$ or $\vec{\tau}=\vec{P} \times \vec{E}$

    Work done in rotation-

     

     

    Then work done by electric force for rotating a dipole through an angle $\theta_2$ from the equilibrium position of an angle $\theta_1$ (As shown in the above figure) is given as

    $
    \begin{aligned}
    & W_{e l e}=\int \tau d \theta=\int_{\theta_1}^{\theta_2} \tau d \theta \cos \left(180^0\right)=-\int_{\theta_1}^{\theta_2} \tau d \theta \\
    & \Rightarrow W_{e l e}=-\int_{\theta_1}^{\theta_2}(P \times E) d \theta=-\int_{\theta_1}^{\theta_2}(P E \operatorname{Sin} \theta) d \theta=P E\left(\cos \Theta_2-\cos \Theta_1\right)
    \end{aligned}
    $


    And So work done by an external force is $W=P E\left(\cos \Theta_1-\cos \Theta_2\right)$
    For example

    $
    \begin{gathered}
    \text { if } \Theta_1=0^{\circ} \text { and } \Theta_2=\Theta \\
    W=P E(1-\cos \Theta) \\
    \text { if } \Theta_1=90^{\circ} \text { and } \Theta_2=\Theta \\
    W=-P E \cos \Theta
    \end{gathered}
    $


    Potential Energy of a dipole kept in Electric field-
    As $\Delta U=-W_{e l e}=W$
    So change in Potential Energy of a dipole when it is rotated through an angle $\theta_2$ from the equilibrium position of an angle $\theta_1$ is given as $\Delta U=P E\left(\cos \Theta_1-\cos \Theta_2\right)$

    $
    \begin{aligned}
    & \text { if } \Theta_1=90^{\circ} \text { and } \Theta_2=\Theta \\
    & \Delta U=U_{\theta_2}-U_{\theta_1}=U_\theta-U_{90}=-P E \cos \Theta
    \end{aligned}
    $


    Assuming $\Theta_1=90^{\circ}$ and $U_{90^{\circ}}=0$
    we can write $U=U_\theta=-\vec{P} \cdot \vec{E}$

    Equilibrium of Dipole-

    1. Stable Equilibrium-

    $
    \begin{aligned}
    & \Theta=0^{\circ} \\
    & \tau=0 \\
    & U_{\min }=-P E
    \end{aligned}
    $
     

    2. Unstable Equilibrium-

    $\begin{aligned} & \Theta=180^{\circ} \\ & \tau=0 \\ & U_{\max }=P E\end{aligned}$

    Note-

    When $\Theta=90^{\circ}$
    then $\tau_{\text {max }}=P E$ and $U=0$
    and it is important to note here that dipole is not in equilibrium since $\tau_{\max } \neq 0$

     

     

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    Electric potential energy of an electric dipole

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