I read a line today and don't get it: "Molecules with mirror symmetry like oxygen, nitrogen, carbon dioxide, and carbon tetrachloride have no permanent dipole moments."
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/diph2o.html
So, why molecules with mirror symmetry have no permanent dipole moment?
Answer
While DumpsterDoofus is right, perhaps this explanation might be helpful.
A dipole is an asymmetric separation of charge, like this: $+ -$. A dipole can have many charges. The total charge must be 0. The center of charge for the $+$ charges and the center of charge for the $-$ charges must be at different places.
A dipole can exert electrical forces on nearby charges, because the nearby charge can be closer to the $-$ than the $+$. $F \propto 1/r^3$
Symmetrical arrangements like this are not dipoles. $+--+$. They are similar, in that they can exert forces. But in this example, $F \propto 1/r^4$. The forces from $+$ and $-$ cancel better than for a dipole, but not perfectly.
A CO2 molecule is a line. O=C=O. The O's are a little $-$, and the C is a little $+$. It can have no dipole moment.
H2O is similar, except that it has a V shape. H2O does have a dipole moment.
The O in the middle is slightly $-$. The H's at the ends are two slightly $+$. The center of $+$ charge is half way between the H's.
Note that a V shape does have a left-right mirror symmetry. This does not prevent a vertical dipole moment.
Inversion symmetry means that if there is something (perhaps a charge) on one side, then there is another identical something on the opposite side. Example shapes include an X, a snowflake, a circle, and a rectangle.
For a distribution of charges with inversion symmetry, the center of $+$ charge and the center of $-$ charge are always at the center. There can be no dipole.
A starfish and a tetrahedron do not have inversion symmetry. Even so, a tetrahedral molecule (carbon tetrachloride) cannot have a dipole.
In summary, there are many symmetries. Some guarantee no dipole moment. Others do not. It is possible for an asymmetrical charge distribution to have no dipole moment.
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