For the same value of n, the penetration power of orbital follows the order (a) s = p = d = f (b) p > s > d > f (c) f < d < p < s (d) s < p < d < f
, for the same shell value (n) the penetrating power of an electron follows this trend in subshells: s>p>d>f And for different values of shell (n) and subshell (l), penetrating power of an electron follows this trend: 1s>2s>2p>3s>3p>4s>3d>4p>5s>4d>5p>6s>4f.... and the energy of an electron for each shell and.
