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    4.

    Separation between the plates of a parallel plate capacitor is dd and the area of each plate is A.A. When a slab of material of dielectric constant kk and thickness t(t<d)t(t < d) is introduced between the plates, its capacitance becomes

    A

    Ξ΅0Ad+t(1βˆ’1k)\frac{{{\varepsilon _0}A}}{{d + t\left( {1 - \frac{1}{k}} \right)}}

    B

    Ξ΅0Ad+t(1+1k)\frac{{{\varepsilon _0}A}}{{d + t\left( {1 + \frac{1}{k}} \right)}}

    C

    Ξ΅0Adβˆ’t(1βˆ’1k)\frac{{{\varepsilon _0}A}}{{d - t\left( {1 - \frac{1}{k}} \right)}}

    D

    Ξ΅0Adβˆ’t(1+1k)\frac{{{\varepsilon _0}A}}{{d - t\left( {1 + \frac{1}{k}} \right)}}

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