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at a glance 4 Bohr’s atomic model Line spectra of hydrogen, helium and mercury 6 Orbiting electrons in hydrogen pictured as de Broglie waves n=3 I n 1913 Danish physicist Niels Bohr (1) published a groundbreaking atomic model. It got round a problem with Rutherford’s 1911 model (P HYSICS R EVIEW Vol. 20, No. 3, pp. 2–5) — a charged particle that accelerates (changes speed and/or direction) emits electromagnetic radiation, so electrons orbiting a nucleus should rapidly lose energy and spiral inwards. 1 2 n=2 Linear and angular momentum mass, m n=1 speed, v radius, r Niels Bohr (1885–1962) linear momentum, ρ = mv Bohr’s first big idea was that angular momentum (2) of orbiting electrons is quantised, and the only possible orbits have: nh (1) L= 2π where n = 1, 2, 3… and h is the Planck constant. This means an orbiting electron can only have certain energies. Bohr’s second big idea was that an electron in a higher energy level moves into a lower one by emitting a single photon (3). Bohr’s model explained atomic line spectra (4) and predicted the wavelengths of hydrogen light (5). 3 Photons and energy levels electron energy E4 n=4 E = ∆E = E4 – E2 photon electron energy energy lost E3 n=3 Dept. of Physics, Imperial College/SPL angular momentum, L = mvr In the 1920s, it was established that a moving particle has wave properties and its de Broglie wavelength, λdeB, is related to its momentum, p: h (2) p An orbiting electron must have a whole number of wavelengths around the circumference of its orbit (6), otherwise the wave will interfere destructively with itself. This approach predicts the same energy levels as Bohr’s model. (You can use Box 2 to show that Equations 1 and 2 are equivalent.) λdeB = 5 Bohr’s model cannot explain everything about atoms and line spectra and it has been superseded by more sophisticated models, but it was a major advance in atomic theory and quantum mechanics. In 1922 Bohr received the Nobel prize for physics. In a long working life at Copenhagen University he developed further theoretical ideas and campaigned for the peaceful use of atomic physics. For more notes on Bohr’s model, and to see how it can be used to calculate the hydrogen wavelengths, visit the web pages linked to this issue of PHYSICS R EVIEW. PhysicsReviewOnline Log on to www.philipallan.co.uk/magazines for a printable PDF of this centre spread. Light emitted by excited hydrogen atoms in a discharge tube photon E = hf = hc energy λ E2 n=2 16 n=1 SPL TopFoto lau fer/Fotolia E1 Physics Review April 2013 17