Question:

(i) Explain the following statements giving reason:

(I) An equipotential surface through a point is normal to the electric field at that point.

(II) When a dielectric is placed in an external electric field, the electric field inside the dielectric is less than that outside it.

(III) The potential difference between the plates of a charged parallel plate capacitor decreases when its plates are brought closer.

(ii) Obtain an expression for the work done to dissociate the system of three charges \(q\), \(-4q\) and \(2q\) placed at the vertices A, B and C respectively of an equilateral triangle of side 'a'.

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Explain each statement using zero work on an equipotential, polarisation of the dielectric, and V = Q/C with C = e0 A/d. For (ii) find U of the three pairs and take W = -U.
Updated On: Oct 21, 2026
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Solution and Explanation

Step 1: Statement (I): equipotential surface is normal to the field:
On an equipotential surface the potential is the same at every point. So the work done in moving a test charge \(q_0\) between two points of the surface is zero.
Take a small displacement \(d\vec{l}\) along the surface. Then \(W = q_0 \vec{E}\cdot d\vec{l} = q_0 E\, dl \cos\theta = 0\).
Since \(q_0\), \(E\) and \(dl\) are not zero, \(\cos\theta = 0\), so \(\theta = 90^{\circ}\). The field is normal to the surface.
If \(E\) had a component along the surface, work would be needed to move a charge on it, and the surface would not be equipotential.

Step 2: Statement (II): field inside a dielectric is smaller:
A dielectric has no free charges, but its molecules get polarised in an external field \(\vec{E}_0\). The positive and negative charges shift slightly in opposite directions.
This leaves a bound charge on the two faces of the slab. The bound charges make an induced field \(\vec{E}_p\) inside the slab, opposite to \(\vec{E}_0\).
\[ E = E_0 - E_p < E_0 \]
So the net field inside is less than the field outside. In fact \(E = E_0/K\), where \(K\) is the dielectric constant.

Step 3: Statement (III): potential difference falls when plates come closer:
A charged capacitor that is not connected to a battery keeps its charge \(Q\) constant.
Its capacitance is \(C = \dfrac{\varepsilon_0 A}{d}\). When the separation \(d\) decreases, \(C\) increases.
\[ V = \frac{Q}{C} = \frac{Qd}{\varepsilon_0 A} \]
With \(Q\) fixed, \(V\) is proportional to \(d\). So the potential difference decreases when the plates are brought closer.

Step 4: Part (ii): set up the three-charge system:
Place \(q\) at A, \(-4q\) at B and \(2q\) at C of an equilateral triangle of side \(a\). Every pair of charges is a distance \(a\) apart.
The work needed to dissociate the system (take all charges to infinity) equals the negative of the potential energy stored in the system.

Step 5: Potential energy of the system:
\[ U = \frac{1}{4\pi\varepsilon_0}\left[\frac{q(-4q)}{a} + \frac{(-4q)(2q)}{a} + \frac{(2q)(q)}{a}\right] \]
\[ U = \frac{1}{4\pi\varepsilon_0 a}\left[-4q^2 - 8q^2 + 2q^2\right] = -\frac{10q^2}{4\pi\varepsilon_0 a} \]

Step 6: Work done to dissociate:
\[ W = -U = \frac{10q^2}{4\pi\varepsilon_0 a} = \frac{5q^2}{2\pi\varepsilon_0 a} \]
The work is positive, because the system is bound (U is negative) and energy must be supplied to pull the charges apart.

Final Answer:
(I) \(E\) is normal to an equipotential surface because no work is done along it. (II) Bound charges reduce the field inside a dielectric. (III) \(V = Q/C\) falls as \(d\) falls at constant \(Q\). The work needed to dissociate the three charges is given below. \[ \boxed{W = \frac{10q^2}{4\pi\varepsilon_0 a}} \]
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