![](../../../Slide%20Images/Didac%2003/Thumbs/D3%20M16.jpg)
Aim: To show the
spatial probability distribution of the py-orbital |
The electron density of the
2p-orbital 2p (n=2, l=1) is not spherical. Each p-orbital is
concentrated along a particular axis, and consists of two parts (called lobes), one on
either side of the nucleus. Since the axes of the orbitals are perpendicular to one
another, there will be three identical orbitals : 2px , 2py
, 2pz. On the left of illustration M16 the radial probability diagram
of 2py orbital is shown. In the middle of the illustration the cross
section of the electron density cloud is shown. It can be seen that the density gradually
increases to a maximum and then decreases again with increasing distance from the nucleus.
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The diagram on the right of illustration M16
gives a representation of the shape of a 2p-orbital corresponding to the boundary surface
enclosing the volume in which there is a 90% chance of finding an electron. Strictly
speaking the lobes do not touch at the origin as can be clearly seen in the cross section
diagram for the electron density. The form drawn here is, however, identical to that found
in many text books. Notes
Illustrations M14, M15, and M16 show the spatial probability distributions for the 1s, 2s,
and 2py orbitals respectively.
It is also possible to define directional probability distributions. These are obtained by
drawing vectors, originating at the centre of the nucleus, where the length of the vector
is proportional to the probability of finding an electron in a given direction. This
produces spheres for the 1s and 2s orbitals and dumb-bells (which do pass through the
origin) for the 2p orbitals.
References:
C.E.
Mortimer, Chemistry, Wadsworth Publishing
Company, Belmont, California.
J.E. Huheey, Inorganic Chemistry, Principles of structure
and reactivity, Harper International SI edition, New-
York. |