Which #d# orbital is specified by #Y(theta,phi) = (5/(8pi))^(1//2) (3cos^2theta - 1)#?
1 Answer
Your angular wave function looks off. Every wave function
- orthogonal (
#int_"allspace" psi_i^"*"psi_jd tau = 0# where#i ne j# ) - normalizable (
#int_"allspace" psi_i^"*"psi_id tau = 1# )
and yours is not. The correct
#color(blue)(Y_(2)^(0)(theta,phi) = (5/(16pi))^"1/2" (3cos^2theta - 1))#
In this case, what we have here is ONLY the angular component of the wave function for the
The full wave function in spherical harmonics is written as the product of the radial and angular components:
#\mathbf(psi_(nlm_l)(vecr,theta,phi) = R_(nl)(vecr)Y_(l)^(m_l)(theta,phi))#
For instance, the full wave function for the
#psi_(3d_(z^2)) = psi_(320)(vecr,theta,phi) = R_(32)(vecr)Y_(2)^(0)(theta,phi)#
#= 1/(81sqrt(6pi))(Z/(a_0))^"3/2" ((Zr)/(a_0))^2e^(-Zr"/"3a_0) (3cos^2theta - 1),# where
#Z# is the atomic number and#a_0# is the Bohr radius (#5.29177xx10^(-11) "m"# ).
This, you would see is quite different and much more complicated.
You did not include
Generally they look like dumbbells along the z-axis with a torus (donut) on the xy-plane. The torus has the OPPOSITE sign to the lobes, and the lobes have the SAME sign as each other.
The
- The
#3d_(z^2)# has#n - l - 1 = 3 - 2 - 1 = 0# radial nodes and#n - 1 = 2# total nodes. Thus, it has two angular nodes.- The
#4d_(z^2)# has#n - l - 1 = 4 - 2 - 1 = 1# radial node and#n - 1 = 3# total nodes. Thus, it has two angular nodes as before.- The
#5d_(z^2)# has#n - l - 1 = 5 - 2 - 1 = 2# radial nodes and#n - 1 = 4# total nodes. Thus, it has two angular nodes as before.- The
#6d_(z^2)# has#n - l - 1 = 6 - 2 - 1 = 3# radial nodes and#n - 1 = 5# total nodes. Thus, it has two angular nodes as before.
So you can see the pattern that the
For instance, here is a picture of the
Now compare that to the
You should notice that the