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CHEM 3308-001 March 13, 2003 MIDTERM EXAM #2: Quantum Angular Momentum, Hydrogenic Atom and Molecular Orbital Theory. 1. Quantum Angular Momentum on a Ring (2-D Rotation); In two dimensions, the total angular momentum operator reduces to the angular momentum operator lˆz along the z-axis: d lˆz i d (1.1) whose eigenfunctions are: 1/ 2 1 ml exp iml 2 (1.2) Then, a) (5 Points): By applying the operator lˆz to its own eigenfunctions ml , obtain the operator’s eigenvalues. State briefly the physical meaning of those eigenvalues. b) (5 Points): Show by explicit integration that two different eigenfunctions: ml and ml are orthogonal. c) (5 Points): Consider the angular momentum eigenfunction with eigenvalue 0 (zero). What kind of motion corresponds to this eigenvalue? From the corresponding eigenfunction, write down the probability density to find the rotating particle on the ring at the position given by the azimuthal angle . State how that probability changes as a function of and discuss whether that 1 change in the probability is consistent with your predicted motion of the particle or not. 2. Hydrogenic Atom I, The 2s Wavefunction: The Hydrogenic 2s wavefunction 2s is: Z 2s 1/ 2 4 2 a0 1 3/ 2 Zr Zr 2 exp a0 2a0 (1.3) where Z is the atom’s atomic number and a0 the Bohr radius. Then, a) (5 Points): State what are the eigenvalues for lˆz and lˆ 2 for an electron in the 2s wavefunction by analyzing the information in its quantum numbers only. b) (5 Points): Determine the number and the position of the radial nodes of the 2s wavefunction as deduced from Eq. 1.3. Then, sketch a 3-D plot of the wavefunction 2s Note: “Sketch” means a plot qualitatively depicted from the information in Eq. 1.3 and your located nodes: you need not calculate anything further to plot! Show the possible nodes on the 3-D plot! 3. Hydrogenic Atom II, Spectroscopic Lines: The energy of a Hydrogenic atom is En Z 2 e4 32 2 0 2n2 ; n 1, 2, 3, 4... (1.4) mN me is the reduced mass, m N the mN me mass of the atom nucleus, me the mass of the electron, e the charge of one electron (in absolute value), and 0 the permitivity of the vacuum. where Z is he atomic number, 2 Then, a) (5 Points) Derive the expression for the wavenumber of the c quantum of light emitted when the electron decays from a state with quantum number n2 to other state with quantum number n1 n2 ; point out the Rydberg constant in your final expression: c En2 En1 hc ???? (1.5) b) (5 Points) Hydrogen has two main isotopes: normal Hydrogen (“Protium”) with mN 1 amu and Deuterium with mN 2 amu . Derive the expression for the ratio of the wavenumbers for a line in v any series Hydrogen ??? Take me mN Ordinary hydrogen is a vDeuterium mixture of normal Hydrogen with a small fraction of Deuterium. How the line series of the emitted light will look like if the Deuterium contribution can be detected? Depict the situation for one (any) of the spectroscopic lines. Be specific! 4. Molecular Orbital Theory: In a diatomic molecule AB , any pair of its (approximate) molecular orbitals (MO) can be expressed as a linear combination of two atomic orbitals: A and B , one per each atom, according to: c A A cB B (1.6) where c A and c B are the coefficients of the linear combination. The combination is a bonding MO and the combination an anti-bonding one. Then, a) (5 Points) In the case of a homonuclear diatomic, the two coefficients must be equal: c A cB N . Then, determine the 3 values of N and N for the bonding and the anti-bonding MO, respectively, by appealing to the normalization of the wavefunctions and . b) (5 Points) Write down the probability densities corresponding to both the wavefunction and . From those expressions and by appealing to physical concepts, explain in detail why the MO is bonding and why the MO is anti-bonding. Refer to the probability density of the two separate atoms in your explanation. Draw plots if necessary. 4