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Rotation in

The special orthogonal group SO(2) is the group of proper rotations in the 2-D space of real vectors, ft2, about an axis z normal to the plane containing x and y. Since there is only one rotation axis z, the notation Rif z) for the rotation of the unit circle in ft2 will be contracted to Rif). Then, for the orthonormal basis (ei e2,  [Pg.182]

But successive rotations about the same axis commute so that the group SO(2) is Abelian with 1-D representations with bases (x + iy)m, m 0, 1, 2,. ..,  [Pg.182]

Restricting m to integer values ensures that the set of functions [Pg.182]

In ft2 there is only one rotation axis, namely z. Rotations about this axis commute  [Pg.183]

I3 is therefore called the infinitesimal generator of rotations about z that comprise SO(2). With r = 1, [Pg.183]


Ship-shaped FPSOs must be designed to weather vane i.e. must have the ability to rotate in the direction of wind or current. This requires complex mooring systems and the connections with the well heads must be able to accommodate the movement. The mooring systems can be via a single buoy or, in newer vessels designed for the harsh environments of the North Sea, via an internal or external turret. Figure 10.33 shows a schematic of the Shell-BP Foinaven FPSO. [Pg.266]

A number of particles perfonn periodic rotations in a ring-shaped contamer with a small opening, through which some particles can escape. Two situations can now be distinguished. [Pg.766]

Case 2. The particles rotate in small packets ( coherently or in phase ). Obviously, the first-order rate law no longer holds. In chapter B2.1 we shall see that this simple consideration has found a deeper meaning in some of the most recent kinetic investigations [21]. [Pg.767]

Variational RRKM theory is particularly important for imimolecular dissociation reactions, in which vibrational modes of the reactant molecule become translations and rotations in the products [22]. For CH —> CHg+H dissociation there are tlnee vibrational modes of this type, i.e. the C—H stretch which is the reaction coordinate and the two degenerate H—CH bends, which first transfomi from high-frequency to low-frequency vibrations and then hindered rotors as the H—C bond ruptures. These latter two degrees of freedom are called transitional modes [24,25]. C2Hg 2CH3 dissociation has five transitional modes, i.e. two pairs of degenerate CH rocking/rotational motions and the CH torsion. [Pg.1016]

Figure B2.3.7. Schematic apparatus of crossed molecular beam apparatus with synclirotron photoionization mass spectrometric detection of the products [12], To vary the scattering angle, the beam source assembly is rotated in the plane of the detector. (By pemrission from AIP.)... Figure B2.3.7. Schematic apparatus of crossed molecular beam apparatus with synclirotron photoionization mass spectrometric detection of the products [12], To vary the scattering angle, the beam source assembly is rotated in the plane of the detector. (By pemrission from AIP.)...
Kiefer J H, Mudipalli P S, Wagner A F and Harding L 1996 Importance of hindered rotations in the thermal dissociation of small unsaturated molecules classical formulation and application to hen and hcch J. Chem. Phys. 105 1-22... [Pg.2151]

Figure C 1.4.7. Spatial variation of the polarization from tire field resulting from two counteriDropagating, circularly polarized fields witli equal amplitude but polarized in opposite senses. Note tliat tire polarization remains linear but tliat tire axis rotates in tire x-y plane witli a helical pitch along tire z axis of lengtli X. Figure C 1.4.7. Spatial variation of the polarization from tire field resulting from two counteriDropagating, circularly polarized fields witli equal amplitude but polarized in opposite senses. Note tliat tire polarization remains linear but tliat tire axis rotates in tire x-y plane witli a helical pitch along tire z axis of lengtli X.
Fig. 8.6 A bond rotation in the middle of a molecule may lead to a large movement at the end. Fig. 8.6 A bond rotation in the middle of a molecule may lead to a large movement at the end.
Place in the tube sufficient organic compound to give subsequently about 0-3 g. of the silver halide, and weigh again. Now allow the small tube to slide carefully down the inclined Carius tube until it finally adopts the position shown in D (Fig. 72). If the compound readily loses halogen in the presence of nitric fumes, the Carius tube should first be rotated in an oblique position to wet the tube for about 10 cm. from the bottom the small tube, if cautiously inserted into the Carius tube, will now come to rest when it first reaches the wet portion of the tube and will thus be held above the main bulk of the acid until the tube is sealed. [Pg.419]

Rotating cone viscometers are among the most commonly used rheometry devices. These instruments essentially consist of a steel cone which rotates in a chamber filled with the fluid generating a Couette flow regime. Based on the same fundamental concept various types of single and double cone devices are developed. The schematic diagram of a double cone viscometer is shown in... [Pg.160]

Orthogonal transformations preserve the lengths of vectors. If the same orthogonal transformation is applied to two vectors, the angle between them is preserved as well. Because of these restrictions, we can think of orthogonal transfomiations as rotations in a plane (although the formal definition is a little more complicated). [Pg.41]

Conservation of orbital symmetry is a general principle that requires orbitals of the same phase (sign) to match up in a chemical reaction. For example, if terminal orbitals are to combine with one another in a cyclixation reaction as in pattern. A, they must rotate in the same dii ection (conrotatory ovei lap). but if they combine according to pattern H. they must rotate in opposite directions (disrotatory). In each case, rotation takes place so that overlap is between lobes of the it orbitals that are of the same sign. [Pg.227]

The properties of a number of sugars are coUected in Table 111,139 the specific rotations in water are included for reference purposes. [Pg.456]

The optically pure salts have rotations in alcohol of [aj, —48-4° [a, ... [Pg.507]

A diatomie moleeule with fixed bond length R rotating in the absenee of any external potential is deseribed by the following Sehrodinger equation ... [Pg.33]

Symmetry tools are used to eombine these M objeets into M new objeets eaeh of whieh belongs to a speeifie symmetry of the point group. Beeause the hamiltonian (eleetronie in the m.o. ease and vibration/rotation in the latter ease) eommutes with the symmetry operations of the point group, the matrix representation of H within the symmetry adapted basis will be "bloek diagonal". That is, objeets of different symmetry will not interaet only interaetions among those of the same symmetry need be eonsidered. [Pg.583]


See other pages where Rotation in is mentioned: [Pg.197]    [Pg.206]    [Pg.240]    [Pg.262]    [Pg.201]    [Pg.270]    [Pg.570]    [Pg.571]    [Pg.580]    [Pg.681]    [Pg.1550]    [Pg.2070]    [Pg.2445]    [Pg.2589]    [Pg.150]    [Pg.503]    [Pg.510]    [Pg.512]    [Pg.337]    [Pg.205]    [Pg.273]    [Pg.109]    [Pg.396]    [Pg.507]    [Pg.597]    [Pg.698]    [Pg.417]    [Pg.418]    [Pg.431]    [Pg.106]    [Pg.75]    [Pg.507]    [Pg.507]    [Pg.642]   


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ASTM Recommendations in the Area of Rotational Rheometry

Additives Used in Rotational Molding

Angular Momentum in Molecular Rotation—The Rigid Rotor

Barrier to Rotation in Ethane

Barrier to internal rotation In ethane

Change in rotation

Core rotation in Tucker3 models

Fast Linear-in-Field Rotation of the Cholesteric Helix

Foaming in rotational molding

Fractional rotational diffusion in potentials

Governing Eulerian Equations in a Rotating Frame

Heat Transfer from a Rotating Cylinder in Simple Shear Flow

Heat Transfer to a Starch Dispersion in an Intermittently Rotated Can

Imaging in the rotating frame

Interference of rotational branches in molecular spectra

Internal rotation in molecules

Internal rotation in small and larger molecules

Internal rotation in small molecules

Longitudinal relaxation in the rotating frame

Longitudinal relaxation time in the rotating frame

Magnetization in the Rotating Frame

Models for Molecular Rotation in Liquids

Molecular rotation in crystals

NMR in the Rotating Frame of Reference

NOE in the rotating frame (ROE)

Numerical simulation of particle fluidization behaviors in a rotating

Optical Rotation in Cuprammonium Solution

Optical rotation in LICS

Other Observables in Rotating Systems

Pendular Ions in FAIMS The Matter of Rotational Hysteresis

Plane Waves in Anisotropic Materials without Optical Rotation

Plane Waves in Materials with Optical Rotation

Plasticizers in rotational molding

Pulsed NMR in the Rotating Frame of Reference

Quantum Mechanical Objects in the MO Framework via Elementary Jacobi Rotations

Railway Axle in Rotating Bending-Shoulder Fillets

Relaxation in the Rotating Frame of Reference

Relaxation in the rotating frame

Relaxation times in the rotating frame

Ring Rotations in Polystyrenes

Rotating Disk in a Finite Gap

Rotating Shaft in Infinite Media

Rotating disk in a sea of fluid

Rotation about Sigma (a) Bonds in Acyclic Alkanes, Alkenes, Alkynes, and Alkyl-Substituted Arenes

Rotation and libration in a fluctuating cell

Rotation in Substituted Ethanes

Rotation in Three Dimensions

Rotation in a plane

Rotation in amides

Rotation in spherical mode

Rotational Barriers in Substituted Phenols

Rotational Diffusion of Liquid Crystals in the Nematic Phase

Rotational Fine Structure in Electronic Band Spectra

Rotational Transitions in Molecules

Rotational barrier in ethane

Rotational barriers in butanes

Rotational freedom and uniqueness in three-way component models

Rotational in radians per second

Rotational or vortex motion in a fluid

Rotational-vibrational bands in the mid-IR

Rotations in Molecules

Rotations in diatomics

Rotations in ethane

Rotations in polyatomics

Rotations in spin space

Scale-Up in Co-Rotating Twin Screw Extruders

Schematic illustration of rotational autoionization in para

Small-molecule rotational diffusion in polymer solutions

Solid-body rotation in a rotating tank

Spin-lattice relaxation in the rotating frame

Spin-lattice relaxation times in rotating

Spin-lattice relaxation times in rotating determined values

Spin-lattice relaxation times in rotating frames

Technique to Solve Blochs Equation in a Rotating Frame Using Fourier-Series Expansion

The Rotating Sphere in a Quiescent Fluid

The Rotation of Molecules in Crystals

The coupled nature of internal rotations in polymers

The statistical mechanics of vibration-rotation spectra in dense phases

Transition state bond rotation in ethane

Translational and rotational dynamics of water molecules in the grooves

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