Molecules rotating

Electronic spectra are almost always treated within the framework of the Bom-Oppenlieimer approxunation [8] which states that the total wavefiinction of a molecule can be expressed as a product of electronic, vibrational, and rotational wavefiinctions (plus, of course, the translation of the centre of mass which can always be treated separately from the internal coordinates). The physical reason for the separation is that the nuclei are much heavier than the electrons and move much more slowly, so the electron cloud nonnally follows the instantaneous position of the nuclei quite well. The integral of equation (BE 1.1) is over all internal coordinates, both electronic and nuclear. Integration over the rotational wavefiinctions gives rotational selection rules which detemiine the fine structure and band shapes of electronic transitions in gaseous molecules. Rotational selection rules will be discussed below. For molecules in condensed phases the rotational motion is suppressed and replaced by oscillatory and diflfiisional motions. 

The shielding at a given nucleus arises from the virtually instantaneous response of the nearby electrons to the magnetic field. It therefore fluctuates rapidly as the molecule rotates, vibrates and interacts with solvent molecules. The changes of shift widi rotation can be large, particularly when double bonds are present. For... 

In the Bom-Oppenlieimer [1] model, it is assumed that the electrons move so quickly that they can adjust their motions essentially instantaneously with respect to any movements of the heavier and slower atomic nuclei. In typical molecules, the valence electrons orbit about the nuclei about once every 10 s (the iimer-shell electrons move even faster), while the bonds vibrate every 10 s, and the molecule rotates... 

C3.3.4 DEDUCING ENERGY TRANSFER MECHANISMS FROM POPULATION AND VELOCITY DISTRIBUTIONS OF THE SCATTERED BATH MOLECULES ROTATIONAL STATE POPULATION DISTRIBUTIONS FOR VIBRATIONAL EXCITATION OF THE BATH... 

When a molecule rotates, IlypcrChem abandons the current contour map because it is no longer valid and you must explicitly request a new contour map via the Graph check box. 

In the case of a polyatomic molecule, rotation can occur in three dimensions about the molecular center of mass. Any possible mode of rotation can be expressed as projections on the three mutually perpendicular axes, x, y, and z hence, three moments of inertia are necessar y to give the resistance to angular acceleration by any torque (twisting force) in a , y, and z space. In the MM3 output file, they are denoted IX, lY, and IZ and are given in the nonstandard units of grams square centimeters. 

As before, when pf i(Rg) (or dpfj/dRa) lies along the molecular axis of a linear molecule, the transition is denoted a and k = 0 applies when this vector lies perpendicular to the axis it is called n and k = 1 pertains. The resultant linear-molecule rotational selection rules are the same as in the vibration-rotation case ... 

In a diatomic or linear polyatomic molecule rotational Raman scattering obeys the selection rule... 

Just as for diatomics, for a polyatomic molecule rotational levels are symmetric (5 ) or antisymmetric (a) to nuclear exchange which, when nuclear spins are taken into account, may result in an intensity alternation with J. These labels are given in Figure 6.24. 

As is the case for diatomic molecules, rotational fine structure of electronic spectra of polyatomic molecules is very similar, in principle, to that of their infrared vibrational spectra. For linear, symmetric rotor, spherical rotor and asymmetric rotor molecules the selection mles are the same as those discussed in Sections 6.2.4.1 to 6.2.4.4. The major difference, in practice, is that, as for diatomics, there is likely to be a much larger change of geometry, and therefore of rotational constants, from one electronic state to another than from one vibrational state to another. 

Models for description of liquids should provide us with an understanding of the dynamic behavior of the molecules, and thus of the routes of chemical reactions in the liquids. While it is often relatively easy to describe the molecular structure and dynamics of the gaseous or the solid state, this is not true for the liquid state. Molecules in liquids can perform vibrations, rotations, and translations. A successful model often used for the description of molecular rotational processes in liquids is the rotational diffusion model, in which it is assumed that the molecules rotate by small angular steps about the molecular rotation axes. One quantity to describe the rotational speed of molecules is the reorientational correlation time T, which is a measure for the average time elapsed when a molecule has rotated through an angle of the order of 1 radian, or approximately 60°. It is indirectly proportional to the velocity of rotational motion. 

Fig. 7-8. Types of motion of a molecule of carbon dioxide, C(>2. A. Translational motion the molecule moves from place to place. B. Rotational motion the molecule rotates about its center of mass. C. Vibrational motion the atoms move alternately toward and away from the center of mass.

Some molecules undergo an internal motion in which one part of the molecule rotates about a bond connecting it with the rest of the molecule. Some examples are... 

In ethane, for example, the two halves of the molecule rotate around the bond so that the molecule passes through eclipsed and staggered conformations and all the intermediate orientations. In methanol, the hydroxyl group swings around the methyl group. 

Hindered Rotation (kT to) With hindered rotation, the potential energy of the internal rotation is restricted by a potential barrier, Vq, whose magnitude varies as the two parts of the molecules rotate past each other in a cyclic fashion. For example, in the molecule H3C-CCI3, the potential varies as the hydrogen atoms on one carbon move past the chlorine atoms on the other. 

FIGURE 5.4 A polar molecule rotating near another polar molecule spends more time in the low-energy orientations (shown shaded) that maximize attractions, and so the net interaction is attractive, but not as strong as it would be if the molecules were not rotating. 

Doubling the separation of polar molecules reduces the strength of the interaction by a factor of 26 = 64, and so dipole-dipole interactions between rotating molecules have a significant effect only when the molecules are very close. We can now start to understand why the kinetic model accounts for the properties of gases so well gas molecules rotate and are far apart for most of the time, so any intermole-cular interactions between them are very weak. Equation 4 also describes attractions between rotating molecules in a liquid. However, in the liquid phase, molecules are closer than in the gas phase and therefore the dipole-dipole interactions are much stronger. 

Polar molecules take part in dipole-dipole interactions, the attraction between the partial charges of their molecules. Dipole-dipole interactions are weaker than forces between ions and fall off rapidly with distance, especially in the liquid and gas phases, where the molecules rotate. 

Enantiomers differ in one physical property chiral molecules display optical activity, the ability to rotate the plane of polarization of light (Section 16.7 and Box 16.2). If a chiral molecule rotates the plane of polarization clockwise, then its mirror-image partner rotates it through the same angle in the opposite direction. 

The question may be asked Just why does a chiral molecule rotate the plane of polarized light Theoretically, the answer to this question is known and in a greatly simplified form may be explained as follows. ... 

Time Resolved Fluorescence Depolarization. In Equation 3, it is assumed that the polarization decays to zero as a single exponential function, which is equivalent to assuming that the molecular shape is spherical with isotropic rotational motion. Multiexponential decays arise from anisotropic rotational motion, which might indicate a nonspherical molecule, a molecule rotating in a nonuniform environment, a fluorophore bound to tbe molecule in a manner that binders its motion, or a mixture of fluorophores with different rotational rates. 

For fixed non-resonant sign, when the dipole moment of a molecule rotates by... 

Synchrotron Radiation Based Perturbed Angular Correlation, SRPAC (Example Whole-Molecule Rotation of FC)... 

In plastic crystals all or a part of the molecules rotate about their centers of gravity. Typically, plastic crystals are formed by nearly spherical molecules, for example hexafluorides like SF6 or MoF6 or white phosphorus in a temperature range immediately below the melting point. Such crystals often are soft and can be easily deformed. 

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