The electric field in a certain region is acting radially outward and is given by E=Ar. A charge contained in a sphere of radius 'a' centered at the origin of the field, will be given by:
Aε₀a²
4πε₀Aa²
4πε₀Aa³
ε₀Aa³
Solution:
From Gauss's law, ∮→E⋅→dS=qenc/ε₀ At r=a, E=Aa ∴∮→E⋅→dS = (Aa)4πa² = qenc/ε₀ →qenc = 4πε₀Aa³