00:01
We're considering a spectral line as the limit in one goes to infinity.
00:06
So it wants us to evaluate this series limit for the linemen series in part a and the balmer series and part b for hydrogen atoms.
00:14
So for the lyman series, the value in two is equal to one.
00:20
And by definition for the balmer series, the value in two is going to be equal to two.
00:24
Of course, to calculate the wavelength, we're going to use the equation that determines wavelength of the spectral line for hydrogen atom.
00:31
So 1 over lambda is equal to the rigberg constant r .1 .07 times 10 to the 7 inverse meters times 1 over n2 squared minus 1 over n1 squared.
00:42
Of course, if n1 goes to infinity, then this value here goes to zero.
00:51
So we can rearrange this equation to solve for lambda, and we find that lambda is equal to n2 squared over.
01:06
Over the rydberg constant.
01:09
So plugging in our value for n2 and the value for the rydberg constant, we find that lambda here is equal to 91 .1 times 10 to minus 9 meters or 91 .1 nanometers.
01:28
I'm going to write it as nanometers, but you could also write it as meters...