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Introduction to SAT II Physics - FreeExamPapers

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The Problem with Rutherford’s Model<br />

Light and other electromagnetic waves are emitted by accelerating charged particles. In<br />

particular, the electrons being accelerated in orbit about the nucleus of an a<strong>to</strong>m release a<br />

certain amount of energy in the form of electromagnetic radiation. If we recall the chapter<br />

on gravity, the radius of an object in orbit is a function of its potential energy. If an<br />

electron gives off energy, then its potential energy, and hence the radius of its orbit about<br />

the nucleus, should decrease. But according <strong>to</strong> Rutherford’s model, any radiating electron<br />

would give off all its potential energy in a fraction of a second, and the electron would<br />

collide with the nucleus. The fact that most of the a<strong>to</strong>ms in the universe have not yet<br />

collapsed suggests a fundamental flaw in Rutherford’s model of electrons orbiting nuclei.<br />

The Mystery of A<strong>to</strong>mic Spectra<br />

Another puzzling phenomenon unexplained by Rutherford’s model, or anything else<br />

before 1913, is the spectral lines we see when looking through a spectroscope. A<br />

spectroscope breaks up the visible light emitted from a light source in<strong>to</strong> a spectrum, so<br />

that we can see exactly which frequencies of light are being emitted.<br />

The puzzling thing about a<strong>to</strong>mic spectra is that light seems <strong>to</strong> travel only in certain<br />

distinct frequencies. For instance, we might expect the white light of the sun <strong>to</strong> transmit<br />

light in an even range of all different frequencies. In fact, however, most sunlight travels<br />

in a handful of particular frequencies, while very little or no light at all travels at many<br />

other frequencies.<br />

Bohr’s Hydrogen A<strong>to</strong>m<br />

Niels Bohr drew on Rutherford’s discovery of the nucleus and Einstein’s suggestion that<br />

energy travels only in distinct quanta <strong>to</strong> develop an a<strong>to</strong>mic theory that accounts for why<br />

electrons do not collapse in<strong>to</strong> nuclei and why there are only particular frequencies for<br />

visible light.<br />

Bohr’s model was based on the hydrogen a<strong>to</strong>m, since, with just one pro<strong>to</strong>n and one<br />

electron, it makes for the simplest model. As it turns out, Bohr’s model is still mostly<br />

accurate for the hydrogen a<strong>to</strong>m, but it doesn’t account for some of the complexities of<br />

more massive a<strong>to</strong>ms.<br />

According <strong>to</strong> Bohr, the electron of a hydrogen a<strong>to</strong>m can only orbit the pro<strong>to</strong>n at certain<br />

distinct radii. The closest orbital radius is called the electron’s ground state. When an<br />

electron absorbs a certain amount of energy, it will jump <strong>to</strong> a greater orbital radius. After<br />

a while, it will drop spontaneously back down <strong>to</strong> its ground state, or some other lesser<br />

radius, giving off a pho<strong>to</strong>n as it does so.<br />

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