# Electron Orbital Shapes

Now, let's look closer at these electron orbitals and their shapes. Remember, we used a two-dimensional plot of the wave function versus x to visualize the standing wave of an electron trapped in one dimension. To visualize the standing waves (or orbitals) of electrons bound to a positively charged nucleus in three dimensions, we will need a four-dimensional plot of the wave function vs. x, y, and z. This can be a bit tricky since our visual perception is limited to three spatial dimensions. So we will need a few tricks to help us visualize the four-dimensional standing waves of the electron in 3 dimension.

## 1s-orbital:

The lowest energy orbital of the hydrogen atom. ## 2s-orbital:

The second harmonic state. Remember that at the node, the probability of finding the electron is zero. In general, an orbital with high n (principal quantum number) (e.g. n = 2, 3, 4...) means that the electron will extend out from the nucleus further, and so will be held less tightly than a 1s electron.

## 2p-orbital:

When n = 2, we have 2 possible values for . The first is ℓ = 0, or 2s orbital, which we just discussed above. The second possibility is ℓ = 1 or the 2 p orbital. For a given value of there are 2 ℓ + 1 possible ml values. So for ℓ = 1, we have m= -1, 0, +1. These three values of m correspond to three different p-orbitals. P-orbitals look like dumbbells along each axis. Instead of a radial node, we have an angular node, which lies along the plane perpendicular to the axis in which the orbital lies. Since the energy, E, of each orbital is a function of only n, then all the n = 2 orbitals (2s, 2px, 2py, 2pz) have the same energy.

## n = 3 orbitals:

For the n=3 orbitals the possible quantum numbers are:

 n=3 ℓ=0 mℓ=0 3s orbital n=3 ℓ=1 mℓ=-1, 0, +1 3p orbitals n=3 ℓ=2 mℓ=-2, -1, 0, +1, +2 3d orbitals

For much nicer three-dimensional renderings of all the atomic orbitals visit Mark Winter's Orbitron site .

#### Homework from Chemisty, The Central Science, 10th Ed.

6.49, 6.51, 6.53, 6.55, 6.57