For 1s, radial part of wave function isΨ(r)​=2(a0​1​)3/2e−a0​r​probability of finding an e− in a spherical shell of thickness, 'dr' at distance 'r' from nucleusp=Ψ(r)2​⋅4πr2dr16πr2(a0​1​)3e−a0​2r​drSo P is zero at r=0 and r=∞.