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RLE-TR-078-047086
RLE-TR-078-047086

TORQUE AND ANGULAR MOMENTUM 73. (11.3) Angular
TORQUE AND ANGULAR MOMENTUM 73. (11.3) Angular

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Rigid Body - GEOCITIES.ws

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mr10Tsol

M.Sc. Chemistry - Jiwaji University
M.Sc. Chemistry - Jiwaji University

1s + 2p
1s + 2p

... “Atom in a Box” can be used to show: (1) Spectral transitions for H atom (levels, energy, wavelength) (2) Static shift of e-density from mixing 2s with 2p (same energy) (3) Oscillation of e-density from mixing orbitals with different energy because of change in relative phase* with time (add, then ...
Example2 - mrdsample
Example2 - mrdsample

D - The University of British Columbia
D - The University of British Columbia

Notes in pdf format
Notes in pdf format

Chapter 10 – Rotation and Rolling
Chapter 10 – Rotation and Rolling

ROTATIONAL MOTION
ROTATIONAL MOTION

Elements for Syllabi
Elements for Syllabi

Document
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University Physics-1 Ch-10 NAME: HOMEWORK CHAPTER 10
University Physics-1 Ch-10 NAME: HOMEWORK CHAPTER 10

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File - Akers Physics

Foreign molecules and ions in beryl obtained by infrared and visible
Foreign molecules and ions in beryl obtained by infrared and visible

ch08_LecturePPT
ch08_LecturePPT

PowerPoint Presentation - Chapter 15 Thermodynamics
PowerPoint Presentation - Chapter 15 Thermodynamics

Does molecular electronics compute?
Does molecular electronics compute?

... To think of molecules as only being a substitute for silicon is limiting. As Mario Ruben of the Karlsruhe Institute of Technology succinctly put it at the recent conference ‘Future Directions in Molecular Electronics’ held in Leiden: “to do Boolean logic with molecules is to do violence against them ...
Circular motion
Circular motion

Chapter 8 Rotational Dynamics continued
Chapter 8 Rotational Dynamics continued

TODAY:
TODAY:

Section 8-2 Center of Mass
Section 8-2 Center of Mass

Physical Chemistry
Physical Chemistry

Laser–Induced Control of Condensed Phase Electron Transfer
Laser–Induced Control of Condensed Phase Electron Transfer

< 1 ... 37 38 39 40 41 42 43 44 45 ... 53 >

Rotational spectroscopy



Rotational spectroscopy is concerned with the measurement of the energies of transitions between quantized rotational states of molecules in the gas phase. The spectra of polar molecules can be measured in absorption or emission by microwave spectroscopy or by far infrared spectroscopy. The rotational spectra of non-polar molecules cannot be observed by those methods, but can be observed and measured by Raman spectroscopy. Rotational spectroscopy is sometimes referred to as pure rotational spectroscopy to distinguish it from rotational-vibrational spectroscopy where changes in rotational energy occur together with changes in vibrational energy, and also from ro-vibronic spectroscopy (or just vibronic spectroscopy) where rotational, vibrational and electronic energy changes occur simultaneously.For rotational spectroscopy, molecules are classified according to symmetry into spherical top, linear and symmetric top; analytical expressions can be derived for the rotational energy terms of these molecules. Analytical expressions can be derived for the fourth category, asymmetric top, for rotational levels up to J=3, but higher energy levels need to be determined using numerical methods. The rotational energies are derived theoretically by considering the molecules to be rigid rotors and then applying extra terms to account for centrifugal distortion, fine structure, hyperfine structure and Coriolis coupling. Fitting the spectra to the theoretical expressions gives numerical values of the angular moments of inertia from which very precise values of molecular bond lengths and angles can be derived in favorable cases. In the presence of an electrostatic field there is Stark splitting which allows molecular electric dipole moments to be determined.An important application of rotational spectroscopy is in exploration of the chemical composition of the interstellar medium using radio telescopes.
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