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  • 1
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Applied mechanics and materials Vol. 10-12 (Dec. 2007), p. 182-186 
    ISSN: 1662-7482
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Because of many advantages that other kinds of bearings can not match, for examplehigh precision and high speed, gas lubricated bearing has been used widely in areas such asultra-precision machine tool and inertia apparatus. The paper introduced an orifice restrictorexternally pressurized spherical gas bearing, which is easily shaped and has bigger stiffness in bothaxial and radial directions. The paper also introduced a bearing force calculation model based onfinite partition of the bearing, in which the influence of the uniform pressure slot also considered
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Applied mechanics and materials Vol. 10-12 (Dec. 2007), p. 732-736 
    ISSN: 1662-7482
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: The influence of parameters to load performances of a high-speed externally pressurizedspherical gas bearing compensated by two-rows of orifices has been studied numerically based onfinite element method (FEM). Reynolds equation governing the flow field in the clearance space inspherical coordinates system is transformed into a analogous style in Descartesian coordinates byparameter substitution, and Galerkin weighted residual method is applied to reduce the order ofderivatives of the transformed equation. Pressure distribution on the gas-film is obtained by solvingof the equation. On the basis of theories, influences of rotating speed, nominal gas-film thicknessand supplying pressure to load carrying capacity and stiffness are analyzed. Comparison ofperformances between hydrostatic and hybrid state of the bearing has also presented
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 6641-6645 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The effect of Renner–Teller coupling between the a˜ 1A1 and b˜ 1B1 states of CH2 on the rotational structure of the a˜ 1A1 bending vibrational levels has been observed. Renner–Teller coupling causes a decrease in the A rotational constant of the a˜ 1A1 (0,5,0) level, at 6400 cm−1 above the zero-point level, compared to the value extrapolated from the (0,v2,0) v2=0–4 levels. Excellent agreement is obtained between the experimentally determined A value for (0,5,0) and that predicted by ab initio calculations of Green et al. [J. Chem. Phys. 94, 118 (1991)]. The effect of Renner–Teller coupling on the A rotational constant of bending levels as low as v2=3 has also been detected. The barrier height to linearity in the a˜ 1A1 state was also estimated by fitting the a˜ 1A1 bending level term values to a harmonic plus Gaussian perturbation potential function, where the effects of orbital angular momentum were explicitly included to account for electronic-rotational coupling in the calculation. The value of 8600±400 cm−1 obtained is in good agreement with the ab initio result of 8800 cm−1. © 1995 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 7832-7835 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Infrared emission from highly vibrationally excited NO2, prepared by collision induced internal conversion, can be detected with 1 cm−1 spectral and 0.5 μs time resolution over the 800–10 000 cm−1 range by time-resolved Fourier transform emission spectroscopy. The energy distribution of vibrationally excited NO2 during collisional deactivation can be extracted from the emission spectra and shows that the energy loss per collision increases dramatically from 〈50 cm−1 below 13 000 cm−1 energy to 1300 cm−1 at 20 000 cm−1 energy.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 8677-8680 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The collisional deactivation of highly vibrationally excited NO2 and CS2 by a variety of buffer gases has been examined by time-resolved Fourier transform IR emission spectroscopy. The results show that there is a dramatic increase in the average energy removed per collision for NO2 excited above ∼10 000 cm−1 and for CS2 above ∼26 000 cm−1. These energies correspond to the origins of the lowest excited A˜ 2B2/B˜ 2B1 states of NO2 and the lowest excited R 3A2 state of CS2. Mixing between these excited electronic states with the ground electronic state enhances collisional relaxation by allowing the electronic transition dipole to contribute to collisional energy transfer. © 1995 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 8554-8563 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Time-resolved Fourier transform infrared emission spectra, recorded after 475 nm excitation of NO2 in a CO2 or N2O bath, show IR emission from collisionally populated vibrational levels of the bath gas. The frequency of the observed bands proves that the emission arises from either the (1,00,1), (0,2l,1), and/or (0,00,2) levels of CO2 or N2O. From the pressure dependence of the emission intensity it was determined that these levels are populated by single collisions with excited NO2. Under typical conditions (1:10 ratio of NO2 to bath gas and 1–2 Torr total pressure) a steady state concentration is reached in our experiments where 0.016±0.006 multiply excited CO2 molecules, or 0.03±0.01 multiply excited N2O molecules were generated per laser excited NO2. A transition dipole coupling model is applied to explain these results, where the resonance conditions for vibration-to-vibration energy transfer are relaxed by extensive vibronic and vibrational couplings in highly excited NO2. In this model the energy-dependent transition dipole of excited NO2 is derived from the time-resolved IR emission spectra. The probability of Δv=1 energy transfer collisions for excited NO2 with CO2 or N2O can be accurately calculated. However, the number of multiply excited species produced (Δv(approximately-greater-than)1) is grossly underestimated. Analysis of the time-resolved data shows that the probability for Δv(approximately-greater-than)1 V–V energy transfer is ca. two orders of magnitude larger than the probability predicted by the dipole coupling model, and that NO2 molecules with energies as low as 5000 cm−1 have a non-negligible probability for exciting the overtone levels of CO2 and N2O. Finally, it was found that the dipole coupling model also underestimates the probability for the ΔE(approximately-greater-than)10 000 cm−1 supercollisions deduced in previous experiments (see Refs. ).
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 2890-2902 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The collisional relaxation of highly vibrationally excited NO2 has been studied for a variety of collision partners (He, Ar, CO, N2, O2, N2O, NO2, CO2, SF6, and toluene) by time-resolved Fourier transform infrared emission spectroscopy. The average energy 〈E〉 of the vibrationally excited NO2 molecules during collisional quenching was obtained from the IR spectra by modeling the ν3 and ν1+ν3 bands, using the known harmonic frequencies and anharmonicity constants. The average amount of energy lost per collision 〈ΔE〉 was determined from the 〈E〉 versus time data. The results show that there is a dramatic increase in the amount of energy transferred for all bath gases at NO2 energies above 10 000–12 000 cm−1, which is near the origin of the NO2 A˜2B2/B˜2B1 states. This threshold in the energy-transfer rate occurs because of strong vibronic coupling between the X˜2A1 and A˜2B2/B˜2B1 electronic states. The increase in vibration-to-vibration (V-V) energy transfer can be understood within the context of the transition dipole coupling model. Vibronic coupling in NO2 produces extensive broadband emission in the IR and near-IR, which enhances the V-V energy-transfer rate by relaxing the resonance conditions in dipole coupling. The V-V energy-transfer probability was calculated using the dipole coupling model, where the transition dipole moment of excited NO2 was directly extracted from the IR emission spectra. These calculations successfully reproduced the observed threshold in the V-V energy transfer probability. The transition dipole coupling model was also used to estimate the relative contribution of V-V versus vibration-to-translation, rotation (V-T,R) energy transfer for NO2 deactivation. The calculations showed that V-T,R energy transfer is the major relaxation channel for triatomic or smaller collision partners. For larger species like SF6, however, V-V energy transfer is the dominant channel. Vibronic coupling may cause an increase in the V-T,R energy-transfer rate by allowing electronic potential related terms, possibly the electronic transition dipole moment, to contribute to the matrix elements responsible for V-T,R energy transfer. © 1997 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 7010-7012 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dispersed fluorescence spectra of the CH2b˜ 1B1→a˜ 1A1'2116 band were recorded by Fourier transform emission spectroscopy for a series of rotational levels in the b˜1 B1 (0,160,0) state. Strong ΔKa=3 transitions were observed with their intensity increasing as J increases in the a˜ 1A1 (0,1,0) state. The observed intensities could be well reproduced by a calculation based on a rigid asymmetric rotor Hamiltonian, in which CH2 was assumed to be linear in the b˜ 1B1 state and bent in the a˜1A1 state. The calculation shows that the intensity of the ΔKa=3 transitions arises from the asymmetry of the a˜ 1A1 state.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 6906-6916 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dispersed fluorescence spectra from the CH2 b˜ 1B1→a˜ 1A1 band were recorded with time-resolution by Fourier transform emission spectroscopy after pulsed excitation of a single rotational level of the b˜ 1B1 (0,160,0) state. Fluorescence observed from the initially excited level and from levels populated by rotational energy changing collisions with the bath gas (ketene) was used to deduce the state-to-state rate constants for rotational energy transfer and the state-resolved rate constants for total collisional removal of b˜ 1B1 CH2. The observed propensity rules for rotational energy transfer—ΔJ=±2, ΔKa=0, and ΔKc=±2—are consistent with a quadrupole–dipole interaction between b˜ 1B1 (0,160,0) CH2 and ketene. The existence of a quadrupole in the intermolecular interaction suggests that the structure of CH2 in the b˜ 1B1 (0,160,0) state, averaged over the time of a collision, must be linear. The state-to-state rotational energy transfer rate constants range from approximately equal to the hard sphere gas kinetic rate to four times the gas kinetic rate, with the largest rate constants between rotational levels with the smallest energy gaps. Examination of fluorescence spectra recorded with polarization analysis shows that rotationally elastic (ΔJ=0)M changing collisions are negligible. State-resolved rate constants for reactive collisions between b˜ 1B1 CH2 and ketene were obtained by subtracting the rotational energy transfer contribution from the total rate constants for collisional removal of b˜ 1B1 CH2 (obtained from a Stern–Volmer analysis). These rate constants vary from one to five times the hard sphere gas kinetic rate, and increase with rotational energy for the levels studied. Their magnitudes show that CH2 is about two times as reactive in its b˜ 1B1 state than its a˜ 1A1 state.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 2469-2472 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dispersed fluorescence spectra from the CH2 b˜ 1B1 state to highly excited vibrational levels of the a˜ 1A1 state were recorded by a new technique, Fourier transform dispersed fluorescence spectroscopy. The spectra obtained clearly show the advantages of using a Fourier transform spectrometer for dispersing fluorescence, namely emission over a wide spectral range can be efficiently detected with high sensitivity and resolution. These advantages allow four new vibrational levels in the CH2 a˜ 1A1 state to be observed; the (2,0,0) and (0,5,0) vibrational overtones and the (1,2,0) and (1,3,0) combination bands. The vibrational term values for these levels are given, along with the harmonic frequencies and anharmonicities for the v1 and v2 modes. From the (0,5,0) term value an improved estimate of the barrier height to linearity in the CH2 a˜ 1A1 state is made.
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