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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
   ATMOSPHERIC ELECTRICITY BY S.S.EDUCATION
   POINTS TO REMEMBER BY S.S.EDUCATION
OTHER AIEEE/IIT/PRE-ENGINEERING TUTORIALS
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   Physics Tutorials for AIEEE IIT Pre Engineering
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EXAMPLE BASED ON ELECTRIC FLUX

Example – 1 If a point charge Q is located at the centre of a cube then find (i) flux through the total surface, of the cube (ii) flux through one surface.
Solution : (i) According to Gauss’s law for closed surface Æ = Q/e0 , (ii) Since cube is a symmetrical figure thus by symmetry the flux through each surface is Æ ‘ = Q/6e0
Example – 2 A point charge +q is located L/2 above the centre of a square having side L. Find the flux through this square.
Solution : The charge q can be supposed to be situated at the centre of a cube having side L with outward flux Æ. In this case the square is one of its face having flux Æ/6

\ flux though the square = (q/6e0)
Example – 3 What is the value of electric flux in SI unit in Y-Z plane of area 2m2, if intensity of electric field is ®E = (5i^ + 2i^) N/C.
Solution: Æ = ®.®dA = (5i^ + 2j^).2i^ = 10 V-m
Example – 4 2mC charge is in some Gaussion surface, given outward flux Æ, what additional charge is needed if we want that 6Æ flux enters into the Gaussian surface.
Solution : According to question


Q = - 14mC
Example – 5 A cylinder of length L and radius b has its axis coincident with the x axis. The electric field in this region ®E = 200i^ . Find the flux through (a) the left end of cylinder (b) the right end of cylinder (c) the cylinder curved surface, (d) the closed surface area of the cylinder.
Solution : from fig. then

(a) Æa = ®E.®A = EAcosq
= 200 x pb2 x cos p
=- 200 pb2
(b) Æb = EA cos 0° = 200 pb2
(c) Æc = EA cos 90° = 0 (d) Æ = Æa + Æb + Æc
= - 200 pb2 + 200 pb2 + 0 = 0


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