Potential Energy of a Charge in an External Field

Physics · Electrostatic Potential And Capacitance · NEET

When a charge q sits at a point where the external potential is V, its potential energy is simply U = qV. This is the work an outside agent does to bring q slowly from infinity (where V = 0) to that point. Memory hook: "U = qV — the field made the potential, the charge just pays the bill."
U = qV : charge q brought from infinity to point P in external field10 V20 V30 V40 V (P)equipotential lines (external field)+qfrom ∞charge placed at PU = qV · W = qΔV
A charge +q brought from infinity (V = 0) to point P sitting on the 40 V equipotential of an external field gains potential energy U = qV. Moving it between two lines costs work W = qΔV, independent of path.

Your doubts, answered

What exactly is an 'external' field here?

External means the field E (and potential V) is made by other source charges that are NOT the charge q you are studying. You are given V at each point; you do not care about the energy of the sources. You only ask: how much energy does q have sitting in this given V? Answer: U = qV. We assume q is so small (or the sources are held fixed) that q does not disturb the sources.

Why is the formula U = qV and not U = kq1q2/r?

Both are correct but for different questions. kq1q2/r is the mutual PE of a PAIR of charges you place yourself (system PE, Section 2.7). U = qV is for ONE charge dropped into a field someone else already made — you are handed the potential V, not the source charges. In NEET, if the question gives you 'a field E' or 'a potential V', use U = qV.

How do I find the work to move a charge from point A to point B?

Work by the external agent = change in PE = q(V_B - V_A) = qΔV. It depends only on the two endpoint potentials, never on the path taken. If A and B are on the same equipotential, ΔV = 0 and work = 0. This is why the electrostatic force is called conservative.

Where does the electron-volt (eV) come from?

Put q = e = 1.6×10⁻¹⁹ C through a potential difference of 1 volt. Energy gained = qV = 1.6×10⁻¹⁹ × 1 = 1.6×10⁻¹⁹ J. This amount is defined as 1 electron-volt (1 eV). So 1 eV = 1.6×10⁻¹⁹ J, and 1 MeV = 1.6×10⁻¹³ J. It is just energy = charge × voltage with a small charge.

Can the potential energy be negative?

Yes. U = qV takes the sign of q and V. A positive charge at a positive-potential point has U > 0; a positive charge at a negative-potential point (near a negative source) has U < 0. A negative charge flips all signs. The zero of PE is at infinity where V = 0.

⚠️ The NEET trap
Work to move a charge from A to B depends on the path or on how the equipotential lines are drawn, so the arrangement with lines closer together needs more work.
Work = qΔV = q(V_B − V_A) depends ONLY on the two endpoint potentials. If A is on the 10 V line and B on the 40 V line in every figure, ΔV = 30 V and the work is the same in all figures, whatever the spacing or path.
🧠 Same start V, same end V → same work. The picture in between is a decoy.

Real NEET questions

2017

Diagrams (a),(b),(c),(d) show regions of equipotentials (10 V, 20 V, 30 V, 40 V) arranged differently. A positive charge q is moved from A to B in each diagram, where A lies on the 10 V line and B on the 40 V line. Which statement is correct?

A · Maximum work is required to move q in figure (c).
B · In all the four cases the work done is the same.
C · Minimum work is required to move q in figure (a).
D · Maximum work is required to move q in figure (b).
Solution: Work done by the external agent = change in potential energy = U_B − U_A = qV_B − qV_A = q(V_B − V_A) = qΔV. Step 1: identify endpoints. In every figure A is on the 10 V equipotential and B is on the 40 V equipotential. Step 2: ΔV = V_B − V_A = 40 − 10 = 30 V in all four cases. Step 3: W = q × 30, the same value regardless of how the lines are spaced or the path taken, because the electrostatic field is conservative. Therefore the work done is identical in all four figures → option B.

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Frequently asked

What is the potential energy of a charge q in an external field?

U = qV, where V is the external potential at the location of q. It equals the work done to bring q slowly from infinity (V = 0) to that point.

Is U = qV the same as the energy of a system of charges?

No. U = qV is for one charge placed in a field made by other sources. System PE (kq1q2/r summed over pairs) is the energy of the charges you assemble yourself. NEET questions that give you a potential or field want U = qV.

What is 1 electron-volt in joules?

1 eV = 1.6×10⁻¹⁹ J. It is the energy an electron (charge e) gains when accelerated through a potential difference of 1 volt, from U = qV.

Does the work to move a charge depend on the path?

No. Work = qΔV = q(V_B − V_A) depends only on the start and end potentials. The electrostatic force is conservative, so the path does not matter.

When is the work done zero?

When the charge moves between two points at the same potential (ΔV = 0), for example along an equipotential surface. Then U does not change and no net work is done by the external agent.