n2 orbitals in each energy level, and n subshells in each energy level.
I assume you kind of recognize quantum numbers...
1. n is the principal quantum number, the energy level. n=1,2,3...
2. l is the angular momentum quantum number, corresponding to the shape of the orbitals of that kind. l=0,1,2,3,..,n−1. That is, lmax=n−1.
3. ml is the magnetic quantum number, corresponding to each orbital of that shape. ml=(−l,−l+1,...,0,..,l−1,l+1). That is, |ml|≤l.
4. ms is the spin quantum number for electrons. ms=±12
For n=4, the maximum l is therefore 4−1=3. Of course, there is more than one value of l for one value of n.
That means:
n=4
l=0
m1=(0)
l=1
ml=(−1,0,+1)
l=2
ml=(−2,−1,0,+1,+2)\
l=3=lmax
ml=(−3,−2,−1,0,+1,+2,+3)
and each ml value corresponds to one orbital. We have 4 subshells in this case; s,p,d,f↔0,1,2,3 for the value of l.
We have an odd number of orbitals per subshell (2l+1), and so:
2(0)+1+2(1)+1+2(2)+1+2(3)+1
=1+3+5+7
=16 orbitals in the n=4 energy level.
If you repeat the process for n=3, you would find lmax=2 and there are 9 orbitals in n=3.
n=3
l=0
mi=(0)
l=1
ml=(−1,0,+1)
l=2=lmax
ml=(−2,−1,0,+1,+2)
and each ml value corresponds to one orbital. We have 3 subshells in this case; s,p,d↔0,1,2 for the value of l.
If you repeat the process for n=2, you would find lmax=1 and there are 4 orbitals in n=2.
n=2
l=0
ml=(0)
l=1=lmax
ml=(−1,0,+1)
and each ml value corresponds to one orbital. We have 2 subshells in this case; s,p↔0,1 for the value of l.
If you repeat the process for n=1, you would find lmax=0 and there is 1 orbital in n=1.
n=1
l=0=lmax
ml=(0)
nd each ml value corresponds to one orbital. We have 1 subshell in this case; s↔0 for the value of l.
Thus, we have n2 orbitals in one energy level, and n subshells in one energy level.