Also by using $I = 4{I_0}{\cos ^2}\frac{\phi }{2}$ ==> $\frac{{{I_1}}}{{{I_2}}} = \frac{{{{\cos }^2}({\phi _1}/2)}}{{{{\cos }^2}({\phi _2}/2)}}$ ==> $\frac{K}{{{I_2}}} = \frac{{{{\cos }^2}(2\pi /2)}}{{{{\cos }^2}\left( {\frac{{\pi /2}}{2}} \right)}} = \frac{1}{{1/2}}$ ==> ${I_2} = \frac{K}{2}.$
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$(a)$ The electric lines of force entering into a Gaussian surface provide negative flux.
$(b)$ A charge ' $q$ ' is placed at the centre of a cube. The flux through all the faces will be the same.
$(c)$ In a uniform electric field net flux through a closed Gaussian surface containing no net charge, is zero.
$(d)$ When electric field is parallel to a Gaussian surface, it provides a finite non-zero flux.
Choose the most appropriate answer from the options given below



