- #1
hideelo
- 91
- 15
I am trying to calculate the density of energy states in a two dimensional box. The way my professor did this is by first calculating the amount of states with their energy less than some energy e and taking its derivative with respect to e. In order to see how many energy states there are with energy less than e we are first calculating the amount of momentum states with a k vector less than some k and then translating it into the corresponding condition for energy.
There is one step in the derivation where my professor makes a jump which I do not understand, and I need some help with. I understand that for some given k vector in 2-dimensions, it has magnitude
k = √(kx2 + kx2 ) where kx = π nx/Lx and the same for y.
she then makes the jump that the amount of states with k vectors of magnitude less than some given k is
(1/4)(πk2)/(π/Lx + π/Ly)
I do not understand how she arrived at this, any help would be appreciated
There is one step in the derivation where my professor makes a jump which I do not understand, and I need some help with. I understand that for some given k vector in 2-dimensions, it has magnitude
k = √(kx2 + kx2 ) where kx = π nx/Lx and the same for y.
she then makes the jump that the amount of states with k vectors of magnitude less than some given k is
(1/4)(πk2)/(π/Lx + π/Ly)
I do not understand how she arrived at this, any help would be appreciated