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Q.(a) Why two electric lines of force/field cannot intersect each other ?

(b) State Coulomb's law, explain its vector form and define S.I unit of electric charge. State two limitations of Coulomb's law. OR
(a) What is the shape of equipotential surface for a given point charge q.
(b) State Gauss's theorem. With the help of diagram, derive an expression for the electric field intensity due to uniformly charged thin spherical shell at a point
(i) outside
(ii) inside
(iii) on the surface of the spherical shell.
Punjab PsebPSEB Punjab Class 12 Board 2018Subjective· 6mImportance★★★★★
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Field lines can't cross because the field direction at any point must be unique; Coulomb's law gives the force between two point charges as F⃗=14πε0q1q2r2r^\vec F=\dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1q_2}{r^2}\hat r, with SI unit of charge the coulomb, and it's strictly valid only for point charges at rest in vacuum/a defined medium.

  1. Why field lines cannot intersect: The tangent to an electric field line at any point gives the direction of the net electric field at that point. If two field lines were to cross at a point, the field at that point would have to point in two different directions simultaneously — which is impossible, since the net electric field at any given point is a single, unique vector (found by vector-adding all contributions there). Hence electric field lines never intersect.
  2. Coulomb's law: The electrostatic force between two point charges q1q_1 and q2q_2 separated by a distance rr (in vacuum) is directly proportional to the product of the charges and inversely proportional to the square of the distance between them, and acts along the line joining them: F=14πε0q1q2r2F=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r^2} where ε0\varepsilon_0 is the permittivity of free space. Vector form: if r^21\hat r_{21} is the unit vector from charge 2 to charge 1, the force on charge 1 due to charge 2 is: F⃗12=14πε0q1q2r2r^21\vec F_{12}=\frac{1}{4\pi\varepsilon_0}\frac{q_1q_2}{r^2}\hat r_{21} This vector form automatically gives an attractive force (pointing toward the other charge) for unlike charges (product q1q2<0q_1q_2<0), and a repulsive force (pointing away) for like charges (product q1q2>0q_1q_2>0), consistent with Newton's third law: F⃗12=−F⃗21\vec F_{12}=-\vec F_{21}. …

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