jstrunk said:
The only coordinate system where the covariant and contravariant bases are the same is Rectangular Coodrinates.
You're right, woops, although the contra and covariant basis vectors are all in the same direction for orthogonal coordinate systems their magnitudes are inverse of each other.
jstrunk said:
I have no idea what reciprocal lattice vectors are or how to find exercises using them.
I was just kind of being optimistic that you might have seen different crystal lattice types that you can then compare to their reciprocal lattice types analytically and geometrically. This is a good way to visualize the changes in the two representations 3-dimensionally with non-orthogonal basis vectors (where the differences between covariance and contravariance is most pronounced, though there are primitive lattice vectors that are orthogonal..) This topic is usually the beginning of any text on solid state physics when performing Fourier analysis of lattice structure (x-ray diffraction).
Basically it's just using the equations linking covariant and contravariant basis vectors:\vec{e}^{1} = \frac{\vec{e}_{2} \times \vec{e}_{3}}{\vec{e}_{1} \circ (\vec{e}_{2} \times \vec{e}_{3})}
\vec{e}^{2} = \frac{\vec{e}_{3} \times \vec{e}_{1}}{\vec{e}_{1} \circ (\vec{e}_{2} \times \vec{e}_{3})}
\vec{e}^{3} = \frac{\vec{e}_{1} \times \vec{e}_{2}}{\vec{e}_{1} \circ (\vec{e}_{2} \times \vec{e}_{3})} to change between a set of non-orthogonal basis vectors that represent a crystal's structure to what the crystals look like in "reciprocal space".
It's just this kind of a thing:
http://www.matter.org.uk/diffraction/geometry/images/lattice_vector.gif
http://www.matter.org.uk/diffraction/geometry/images/r_lattice_vector.gif
I dunno, I'm thinking my suggestion is too far from helpful ._. It's too complicated for what looks to be not a lot of enlightenment :/ I remembered it being more enlightening than it's turning out to be.. Though I was trying to appeal from something in physics rather than just straight mathematics.