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Simple Nature - Light and Matter

Simple Nature - Light and Matter

Simple Nature - Light and Matter

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the electron is close to the nucleus it has a lower electrical energy,a higher kinetic energy, <strong>and</strong> a higher momentum.Between each ring of peaks in this wavefunction is a nodal circle,i.e., a circle on which the wavefunction is zero. The full threedimensionalwavefunction has nodal spheres: a series of nested sphericalsurfaces on which it is zero. The number of radii at which nodesoccur, including r = ∞, is called n, <strong>and</strong> n turns out to be closelyrelated to energy. The ground state has n = 1 (a single node onlyat r = ∞), <strong>and</strong> higher-energy states have higher n values. Thereis a simple equation relating n to energy, which we will discuss insubsection 13.4.4.The numbers n <strong>and</strong> l, which identify the state, are called itsquantum numbers. A state of a given n <strong>and</strong> l can be orientedin a variety of directions in space. We might try to indicate theorientation using the three quantum numbers l x = L x /, l y = L y /,<strong>and</strong> l z = L z /. But we have already seen that it is impossible toknow all three of these simultaneously. To give the most completepossible description of a state, we choose an arbitrary axis, say thez axis, <strong>and</strong> label the state according to n, l, <strong>and</strong> l z . 6Angular momentum requires motion, <strong>and</strong> motion implies kineticenergy. Thus it is not possible to have a given amount of angularmomentum without having a certain amount of kinetic energy aswell. Since energy relates to the n quantum number, this meansthat for a given n value there will be a maximum possible . It turnsout that this maximum value of equals n − 1.In general, we can list the possible combinations of quantumnumbers as follows:n can equal 1, 2, 3, . . .l can range from 0 to n − 1, in steps of 1l z can range from −l to l, in steps of 1Applying these rules, we have the following list of states:n = 1, l = 0, l z = 0 one staten = 2, l = 0, l z = 0 one staten = 2, l = 1, l z = −1, 0, or 1 three states. . .self-check JContinue the list for n = 3. ⊲ Answer, p. 929Figure e on page 882 shows the lowest-energy states of the hydrogenatom. The left-h<strong>and</strong> column of graphs displays the wavefunctionsin the x − y plane, <strong>and</strong> the right-h<strong>and</strong> column shows theprobability distribution in a three-dimensional representation.d / The energy of a state inthe hydrogen atom depends onlyon its n quantum number.6 See page 889 for a note about the two different systems of notations thatare used for quantum numbers.Section 13.4 The Atom 881

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