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<strong>www</strong>.<strong>GOALias</strong>.<strong>blogspot</strong>.<strong>com</strong>Electrostatic Potentialand CapacitanceOuter region II (region below the plate 2),E = σ σ02ε− 2ε= (2.40)0 0In the inner region between the plates 1 and 2, the electric fields dueto the two charged plates add up, givingσ σ σ QE = + = =2ε 2ε ε ε A(2.41)0 0 0 0The direction of electric field is from the positive to the negative plate.Thus, the electric field is localised between the two plates and isuniform throughout. For plates with finite area, this will not be true nearthe outer boundaries of the plates. The field lines bend outward at theedges – an effect called ‘fringing of the field’. By the same token, σ will notbe strictly uniform on the entire plate. [E and σ are related by Eq. (2.35).]However, for d 2

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