An electric dipole in an electric field experiences forces and torques due to the interaction with the field. Let's analyze the scenarios:
Force (F) on the Dipole: The force on a dipole in a non-uniform electric field is generally not zero. This is because the strength of the electric field varies at different points in space, leading to a net force on the dipole.
Torque (τ) on the Dipole: Torque depends on the angle between the dipole moment (p) and the electric field (E). The torque τ is given by:
\(τ = pE sin θ\)
where θ is the angle between the dipole moment and the electric field. If the dipole moment is parallel to the electric field, θ is 0, making sin θ = 0. This results in:
\(τ = 0\)
Conclusion: For a dipole in a non-uniform electric field, with the dipole moment parallel to the field, the force F is non-zero (F ≠ 0), while the torque τ is zero (τ = 0).
Correct Answer: \(F ≠ 0, τ = 0\)
An electric dipole consists of two equal and opposite charges, +q and -q, separated by a small distance 2l. The dipole moment p is defined as p = q * (2l) hat-p, where hat-p points from the negative to the positive charge. Here, the dipole moment is parallel to the non-uniform electric field.
The torque tau on a dipole in an electric field E is given by the cross product:
τ = p x E
The magnitude of the torque is:
τ = p * E * sin(theta)
Here, theta is the angle between p and E. Since the dipole moment is parallel to the field, theta = 0 degrees. So:
sin(0 degrees) = 0
τ = p * E * sin(0 degrees) = 0
Therefore, the torque τ = 0. This makes sense—when the dipole is aligned with the field, there’s no rotational effect!
The net force on a dipole in an electric field is given by:
F = (p dot del) E
In a uniform field, E is constant, so del E = 0, and the force F = 0. But in a non-uniform field, E varies with position, so del E is not zero, leading to a net force.
Let’s use an example: Suppose the field is E = k * x i-hat, and the dipole is aligned with the field, so p = p i-hat. The gradient of the field is:
del E = partial derivative of (k * x) with respect to x i-hat = k i-hat
The force is:
F = (p dot del) E
p dot del = p partial derivative with respect to x
F = p * k i-hat
Since k is not zero, the force F is not zero. This shows that in a non-uniform field, the dipole experiences a net force (F is not zero).
A common mistake is thinking the net force on a dipole is always zero. That’s only true in a uniform field! In a non-uniform field, the field strength differs at the +q and -q charges, so the forces don’t cancel out, resulting in a net force.
From our calculations:
- Torque τ = 0, because the dipole is parallel to the field.
- Force F is not zero, because the field is non-uniform.
The correct option is:
B. F is not zero, τ = 0
The net force on the dipole is non-zero (F is not zero) due to the non-uniform electric field, and the torque is zero (τ = 0) because the dipole moment is parallel to the field. The correct answer is B. F is not zero, τ = 0