Scaling of Emission Wavelengths in Balmer Series for ##Li^{2+}##?

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Homework Help Overview

The discussion revolves around the scaling of emission wavelengths in the Balmer series for the lithium ion, ##Li^{2+}##, which is a hydrogen-like atom. Participants are exploring how the emission wavelengths relate to the nuclear charge, Z, and are attempting to derive expressions for the longest and shortest wavelengths in the series.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are attempting to derive the energy levels of hydrogen-like atoms and relate them to emission wavelengths. There is a focus on the Balmer series, particularly the transition from higher energy states to the ##n=2## state. Questions arise regarding the calculation of maximum and minimum wavelengths and the interpretation of energy differences between states.

Discussion Status

Some participants have provided guidance on using energy differences to find wavelengths, while others are questioning the correctness of their calculations and constants. There is an ongoing exploration of how to apply the derived equations to the specific case of the Balmer series.

Contextual Notes

Participants are navigating the complexities of the equations involved and the implications of the nuclear charge on the emission wavelengths. There is uncertainty regarding the correct application of energy differences and the interpretation of results, particularly in relation to the signs of the energy values.

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Homework Statement


The emission wavelengths of hydrogen-like atoms are related to nuclear charge. How do they scale as a function of Z? What are the longest and shortest wavelengths in the Balmer series for ##Li^{2+}##?

Homework Equations


##E_n = -\frac{R}{n^2}## (1)

##a_0 = \frac{\hbar^2}{Zme^2}## (2)

From (2), ##\hbar^2 = a_0Zme^2## (3)

##\alpha = \frac{Ze^2}{\hbar c}## (4)

##R = \frac{1}{2} mc^2 \alpha^2## (5)

The Attempt at a Solution


I started by trying to find an expression for the energy levels of hydrogen-like atoms. Substituting (5) into (1) gives
##E_n = -\frac{mc^2\alpha^2}{2n^2}##
Substitute in (4):
##E_n = -\frac{mZ^2e^4}{2\hbar^2 n^2}##
Sub in (3):
##E_n = -\frac{mZ^2e^4}{2Za_0me^2 n^2}##

Simplifying, ##E_n = -\frac{Ze^2}{2a_0n^2}##. This can be related to wavlength via ##E_n = \frac{hc}{\lambda}##, so emission and absorption wavelengths of hydrogenic atoms are related to nuclear charge Z by the function

##\lambda = -\frac{2hca_0n^2}{Ze^2}##

But I have no idea how to answer the bit about the Balmer series because n=2 and Z=3, so based on my equation isn't there only going to be one answer? How do I get minimum/maximum wavelengths?
 
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Kara386 said:
But I have no idea how to answer the bit about the Balmer series because n=2 and Z=3, so based on my equation isn't there only going to be one answer? How do I get minimum/maximum wavelengths?
In the Balmer series the final state is an ##n=2## state. The initial state may be anything from ##n=3## to ##n=\infty##. You need to find the energy difference between these states.
 
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Incand said:
In the Balmer series the final state is an ##n=2## state. The initial state may be anything from ##n=3## to ##n=\infty##. You need to find the energy difference between these states.
So I use the equation for ##E_n## I found and do ##E_3-E_2## for the maximum wavelength? This gives a negative answer though, can I just multiply that answer by ##-1##? Or do ##E_2-E_3##?
 
##E_3-E_2## is positive from your formula since you got a minus sign in it. That is ##-1/9 > -1/4##.
I don't know if all your other constants are correct but you can always compare your answer to the Rydberg formula https://en.wikipedia.org/wiki/Rydberg_formula
 
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