The spectrum of hydrogen · Physics Class 11–12 | StemPy Lab
Course 25.3·Lesson 3 of 3
The spectrum of hydrogen
Hot gases give out only certain wavelengths. For hydrogen, λ1=R(nf21−ni21)
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A fingerprint in light
Pass the light of a hot solid through a prism. You see a smooth band of colours, a continuous spectrum. Do the same with a glowing gas, and you see only a few bright lines on a dark background. That is an emission line spectrum.
Now shine the light of a hot solid through a cool gas, and look at it through a prism. The band is crossed by dark lines. That is an absorption spectrum. The dark lines are at the same wavelengths as the bright lines of the same gas. Each atom takes in the colours it can also give out.
Every element has its own set of lines, so a spectrum is a fingerprint. Dark lines in sunlight showed that the Sun holds hydrogen, sodium and many other elements. In 1868 a new line in the solar spectrum led to the discovery of helium, on the Sun, before anyone found it on Earth.
The formula for hydrogen
In 1885 Johann Balmer found that four lines of hydrogen in the visible region obey a simple rule. Later Johannes Rydberg put every line into one formula:
λ1=R(nf21−ni21)ni=nf+1,nf+2,…
Here R=1.097×107m−1 is the Rydberg constant. For each nf we get a series of lines, from the jumps ni→nf.
An energy-level diagram of hydrogen. Six black horizontal lines mark the levels n = 1 to n = 6, with energies of minus 13.60, minus 3.40, minus 1.51, minus 0.85, minus 0.54 and minus 0.38 electronvolts, and a dashed line at 0 electronvolts for a free electron. The heights are not to scale: the real levels crowd together near zero. Five purple arrows run down from levels 2 to 6 to n = 1, the Lyman series, in the ultraviolet. Four teal arrows run down to n = 2, the Balmer series, in the visible. Three red arrows run down to n = 3, the Paschen series, and two dark red arrows run to n = 4, the Brackett series, all infrared. A key on the right names each series.
Where Bohr's model gives the formula
A jump gives a photon of energy Ei−Ef=13.6eV(nf21−ni21). Divide by hc to find λ1. So the constant is
That is the value that Rydberg measured. It was the first great success of Bohr's model.
The five series
Each series has a name, a lowest level nf and a region of the spectrum:
Lyman, nf=1: ultraviolet, from 91 nm to 122 nm.
Balmer, nf=2: mostly visible, from 365 nm to 656 nm.
Paschen, nf=3: infrared, from 820 nm to 1875 nm.
Brackett, nf=4: infrared, from 1459 nm to 4051 nm.
Pfund, nf=5: infrared, from 2279 nm to 7458 nm.
A chart of the spectral lines of hydrogen against wavelength on a scale where each step is twice the last, from 91 to 8000 nanometres. A rainbow band marks the visible region from 400 to 700 nanometres, a pale violet region to its left is the ultraviolet, and a pale red region to its right is the infrared. Five rows show five series. The Lyman series lies in the ultraviolet, with its limit at 91 nanometres. The Balmer series has a red, a cyan, a blue and a violet line in the visible region, and its limit at 365 nanometres. The Paschen, Brackett and Pfund series lie in the infrared, with limits at 820, 1459 and 2279 nanometres. In every row the lines crowd together towards the series limit, which is marked by a dotted line.
In every series the lines crowd together as ni grows. They stop at the series limit, the shortest wavelength of the series. It comes from a jump from ni=∞:
λlimit1=nf2R
The Balmer series is the only one with lines in the visible region. Its four visible lines are red at 656 nm, blue-green at 486 nm, violet-blue at 434 nm and violet at 410 nm.
Choose nf=3. Is the first line shorter or longer than for nf=2? Now set Z=2. Where do the lines move, and by what factor?
Ions with one electron
For an ion with one electron, R becomes RZ2:
λ1=RZ2(nf21−ni21)
For He+, Z=2 and Z2=4. Take the jump ni=4 to nf=2:
λ1=4R(41−161)=4R×163=43R
That is exactly the value of the first Lyman line of hydrogen, R(1−41). The wavelength is 121.5nm. In general, a jump of He+ between the levels 2ni and 2nf matches a jump of hydrogen between ni and nf. The other lines of He+ are new.
Practise with new numbers
Try it in Python
The program prints the first lines and the limit of all five series of hydrogen.
Common mistakes
Turning the formula upside down. The formula gives λ1, not λ.
Using n1 in place of n21. The levels are squared.
Taking the first line as the shortest. The first line has the longest wavelength. The shortest is the limit.
Forgetting Z2 for an ion. The lines of He+ have wave numbers four times larger than the matching jump of hydrogen.
Remember these
Emission line spectrum from a glowing gas. Absorption spectrum: dark lines at the same wavelengths.
λ1=R(nf21−ni21), R=1.097×107m−1. For an ion, replace R by RZ2.
Series by lowest level: Lyman 1, Balmer 2, Paschen 3, Brackett 4, Pfund 5.
Lyman: ultraviolet. Balmer: visible. The others: infrared.
Series limit: λ=Rnf2.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
Why does each element have its own line spectrum?
Which series of hydrogen lies partly in the visible region, and on which level do its jumps end?
Which jump gives the limit of the Balmer series?
A jump of He+ from n=8 to n=4 gives a wavelength that is also found in hydrogen. Which jump of hydrogen is it?
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