Potential Due to a System of Charges and an Electric Dipole
The potential at a point due to a system of charges is the algebraic sum of potentials due to individual charges. For an electric dipole, potential depends on distance from the dipole and the angle with its axis.
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Student-friendly explanation
Superposition is simpler for potential than for field because potential is scalar. For charges q1, q2, q3 at distances r1, r2, r3 from a point, V = k(q1/r1 + q2/r2 + q3/r3). For a short dipole, V = k p cos theta/r^2, where p is dipole moment and theta is the angle from the dipole axis. On the axial line, potential is non-zero; on the equatorial line, the potentials due to +q and -q cancel.
How to write this in exams
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Start with the exact idea
The potential at a point due to a system of charges is the algebraic sum of potentials due to individual charges. For an electric dipole, potential depends on distance from the dipole and the angle with its axis.
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Then show how to use it
List each charge and its distance from the point; write each kq/r term with sign; add algebraically; for dipole questions, identify theta; use cos theta; apply axial or equatorial simplification only when the geometry matches.
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Add one concrete example
At a point on the perpendicular bisector of a dipole, the distances from +q and -q are equal. Their potentials are equal in magnitude and opposite in sign, so the net potential is zero.
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Avoid this incomplete answer
Adding magnitudes only gives a wrong positive potential for systems containing negative charges.
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Quick check
Why is the potential zero at a point on the equatorial line of an electric dipole?
The point is equally distant from +q and -q, so the potentials kq/r and -kq/r have equal magnitude and opposite signs. Their algebraic sum is zero.
Answer writing and exam use
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