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ATM-01

Rydberg formula

Hydrogen series lines.

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AtomicRydberg

Governing equation

1/λ=R(1/n12−1/n22)1/\lambda=R(1/n_1^2-1/n_2^2)

n2∈[2,12]n_2 \in \left[2, 12\right]

where

n_1
n1 (—)
n_2
n2 (—)
\lambda
Wavelength (nm)

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ATM-01 · spectrum
00:0 / 00:08
①

Governing law — red

1/λ=R(1/n12−1/n22)1/\lambda=R(1/n_1^2-1/n_2^2)

n2∈[2,12]n_2 \in \left[2, 12\right]

n2=2n_2 = 2λ=0\lambda = 0

②

Domain of the variable — blue

n_2_{\min} = 2,\quad n_2_{\max} = 12

n2∈[2,12]n_2 \in \left[2, 12\right]

n2=2n_2 = 2n2=2n_2 = 2

③

Response curve — green

1/λ=R(1/n12−1/n22)1/\lambda=R(1/n_1^2-1/n_2^2)

n2∈[2,12]n_2 \in \left[2, 12\right]

n2=2n_2 = 2λ=0\lambda = 0

④

Rate of change — amber

dλdn2\frac{\mathrm{d}\lambda}{\mathrm{d}n_2}

n2∈[2,12]n_2 \in \left[2, 12\right]

n2=2.063n_2 = 2.063λ′=25233.2\lambda^{\prime} = 25233.2

Lecture brief

Historical brief

Balmer, Rydberg, Bohr (1913), fine structure, Zeeman and Stern–Gerlach built the spectrum of one atom. The lab computes levels, selection and magnetic splitting. This sheet (ATM-01 — Rydberg formula) is the form associated with Rydberg. Working symbols: n1n_1, n2n_2 →\rightarrow λ\lambda. Hydrogen series lines.

Purpose

Purpose: compute λ\lambda from n1n_1, n2n_2 in Atomic physics via 1/λ=R(1/n12−1/n22)1/\lambda=R(1/n_1^2-1/n_2^2) Hydrogen series lines. Use it when a real atomic physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given n1=2.000 —n_1 = 2.000\,\mathrm{—}, n2=4.000 —n_2 = 4.000\,\mathrm{—}, the governing relation 1/λ=R(1/n12−1/n22)1/\lambda=R(1/n_1^2-1/n_2^2) yields λ=486.01 nm\lambda = 486.01\,\mathrm{nm}. Hydrogen series lines. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Wavelength \lambda486.01 nm
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ATM-01 · spectrum
00:0 / 00:08

Narration of this film

Hydrogen series lines.

Hydrogen series lines.

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