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A tiny electric dipole of dipole moment ...

A tiny electric dipole of dipole moment `vecP = P_0hatj` is placed at point (l,0). There exists an electric field `vecE = 2ax^2hati + (2by^2 + 2cy)hatj`.

A

Force on dipole is `2P_0ahati`.

B

Force on dipole is `2P_0bhati`.

C

Force on dipole is `2P_0chatj`.

D

Force on dipole is `-2P_0chatj`.

Text Solution

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The correct Answer is:
To solve the problem, we need to find the force acting on the electric dipole placed in the given electric field. The dipole moment is given as \(\vec{P} = P_0 \hat{j}\) and the electric field is given as \(\vec{E} = 2a x^2 \hat{i} + (2b y^2 + 2cy) \hat{j}\). The dipole is placed at the point \((l, 0)\). ### Step 1: Identify the components of the dipole moment and electric field The dipole moment \(\vec{P}\) has components: - \(P_x = 0\) (since it only has a \(\hat{j}\) component) - \(P_y = P_0\) The electric field \(\vec{E}\) has components: - \(E_x = 2a x^2\) - \(E_y = 2b y^2 + 2cy\) ### Step 2: Calculate the force on the dipole The force \(\vec{F}\) on a dipole in an electric field is given by: \[ \vec{F} = P_x \frac{\partial E_x}{\partial x} + P_y \frac{\partial E_y}{\partial y} \] ### Step 3: Evaluate the force in the x-direction Since \(P_x = 0\): \[ F_x = P_x \frac{\partial E_x}{\partial x} = 0 \] ### Step 4: Evaluate the force in the y-direction Now we need to calculate \(F_y\): \[ F_y = P_y \frac{\partial E_y}{\partial y} \] Substituting \(P_y = P_0\): \[ F_y = P_0 \frac{\partial E_y}{\partial y} \] ### Step 5: Differentiate \(E_y\) with respect to \(y\) The expression for \(E_y\) is: \[ E_y = 2b y^2 + 2cy \] Differentiating with respect to \(y\): \[ \frac{\partial E_y}{\partial y} = \frac{\partial}{\partial y}(2b y^2 + 2cy) = 4by + 2c \] ### Step 6: Substitute the coordinates of the dipole The dipole is located at the point \((l, 0)\), so we substitute \(y = 0\): \[ \frac{\partial E_y}{\partial y} \bigg|_{y=0} = 4b(0) + 2c = 2c \] ### Step 7: Calculate \(F_y\) Now substituting back into the expression for \(F_y\): \[ F_y = P_0 (2c) = 2P_0 c \] ### Step 8: Write the final force vector Since \(F_x = 0\) and \(F_y = 2P_0 c\), we can write the force vector as: \[ \vec{F} = 0 \hat{i} + 2P_0 c \hat{j} = 2P_0 c \hat{j} \] ### Final Answer The force on the dipole is: \[ \vec{F} = 2P_0 c \hat{j} \] ---

To solve the problem, we need to find the force acting on the electric dipole placed in the given electric field. The dipole moment is given as \(\vec{P} = P_0 \hat{j}\) and the electric field is given as \(\vec{E} = 2a x^2 \hat{i} + (2b y^2 + 2cy) \hat{j}\). The dipole is placed at the point \((l, 0)\). ### Step 1: Identify the components of the dipole moment and electric field The dipole moment \(\vec{P}\) has components: - \(P_x = 0\) (since it only has a \(\hat{j}\) component) - \(P_y = P_0\) The electric field \(\vec{E}\) has components: ...
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