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Electrostatics Tutorials
   ELECTRIC CHARGE BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTRIC CHARGE BY S.S.EDUCATION
   COULOMB’S LAW BY S.S.EDUCATION
   PROBLEM SOLVING TRICKS BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTROSTATICS FORCE BY S.S.EDUCATION
   ELECTROSTATIC FIELD BY S.S.EDUCATION
   ELECTROSTATIC LINES OF FORCE BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTRIC LINES OF FORCE BY S.S.EDUCATION
   ELECTRIC FIELD DUE TO A POINT CHARGE BY S.S.EDUCATION
   SUPERPOSITION OF ELECTRIC FIELDS BY S.S.EDUCATION
   ELECTRIC FIELD INTENSITY ON THE AXIS OF A UNIFORMLY CHARGED RING BY S.S.EDUCATION
   SPECIAL CASES BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTRIC FIELD BY S.S.EDUCATION
   ELECTRIC FLUX BY S.S.EDUCATION
   GAUSS LAW BY S.S.EDUCATION
   APPLICATION OF GAUSS’S LAW BY S.S.EDUCATION
   EXAMPLE BASED ON ELECTRIC FLUX BY S.S.EDUCATION
   ELECTRIC POTENTIAL AND POTENTIAL ENERGY BY S.S.EDUCATION
   ELECTRIC POTENTIAL BY S.S.EDUCATION
   POTENTIAL DIFFERENCE BY S.S.EDUCATION
   RELATION BETWEEN E AND ELECTRIC POTENTIAL BY S.S.EDUCATION
   ELECTRIC POTENTIAL DUE TO POINT CHARGES BY S.S.EDUCATION
   POTENTIAL DUE TO A CHARGED SPHERICAL SHELL BY S.S.EDUCATION
   POTENTIAL DUE TO A CHARGED CONDUCTING SPHERE BY S.S.EDUCATION
   POTENTIAL DUE TO A CHARGED NON-CONDUCTING SPHERE BY S.S.EDUCATION
   POTENTIAL DUE TO A RING AT A POINT LYING ON ITS AXIS BY S.S.EDUCATION
   EQUIPOTENTIAL SURFACE BY S.S.EDUCATION
   ELECTRIC STRENGTH BY S.S.EDUCATION
   ELECTRIC POTENTIAL ENERGY BY S.S.EDUCATION
   ELECTRON VOLT BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTRIC POTENTI AL BY S.S.EDUCATION
   EXAMPLES BASED ON ELECTRIC POTENTIAL ENERGY BY S.S.EDUCATION
   ELECTRIC DIPOLE BY S.S.EDUCATION
   ELECTRIC FIELD AT AN AXIAL POINT BY S.S.EDUCATION
   ELECTRIC FIELD AT AN EQUATORIAL POINT BY S.S.EDUCATION
   ELECTRIC FIELD BY S.S.EDUCATION
   FORCE AND TORQUE ON A DIPOLE PLACED BY S.S.EDUCATION
   ELECTRIC POTENTIAL DUE TO A DIPOLE BY S.S.EDUCATION
   POTENTIAL ENERGY OF A DIPOLE BY S.S.EDUCATION
   EXAMPLES BASED ON DIPOLE SYSTEM BY S.S.EDUCATION
   CHARGED LIQUID DROP BY S.S.EDUCATION
   EXAMPLE BASED ON CHARGED LIQUID DROP BY S.S.EDUCATION
   FORCE ON A CHARGED SURFACEBY S.S.EDUCATION
   EQUILIBRIUM OF A CHARGED SOAP BUBBLE BY S.S.EDUCATION
   MOTION OF A CHARGED PARTICLE IN ELECTRIC FIELD BY S.S.EDUCATION
   EXAMPLES BASED ON MOTION OF A CHARGED PARTICLE BY S.S.EDUCATION
   ELECTROSTATIC BEHAVIOUR OF CONDUCTORS BY S.S.EDUCATION
   INSULATORS BY S.S.EDUCATION
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EXAMPLES BASED ON ELECTRIC LINES OF FORCE

Example – 1 A Solid metallic sphere is placed in a uniform electric field. Which of the lines A, B, C and D shows the correct path and why ?

Solution : Path (A) is wrong as lines of force do not start or end normally on the surface of a conductor. Path (B) and (C) are wrong as lines of force should not exist inside a conductor. Also lines of froce are not normal to the surface of conductor. Path (D) represents the correct situation as here line of force does not exist inside the conductor and starts and ends normally on its surface.
Example – 2 A metallic slab is introduced between the two plates of a charged parallel plate capacitor. Sketch the electric lines of force between the plates.

Solution : Keeping in mind the following properties :
1. Lines of force start from positive charge and end on negative charge.
2. Lines of force start and end normally on the surface of a conductor.
3. Lines of force do not exist inside a conductor (as field inside a conductor is zero)
The field lines between the plates are as shown in the figure.


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