Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $
Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variati...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Hubschmid, W. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Systematik: |
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| Anmerkung: |
© Springer-Verlag 2010 |
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| Übergeordnetes Werk: |
Enthalten in: Applied physics. B, Lasers and optics - Springer-Verlag, 1981, 103(2010), 4 vom: 17. Dez., Seite 933-939 |
|---|---|
| Übergeordnetes Werk: |
volume:103 ; year:2010 ; number:4 ; day:17 ; month:12 ; pages:933-939 |
| Links: |
|---|
| DOI / URN: |
10.1007/s00340-010-4341-y |
|---|
| Katalog-ID: |
OLC2074302894 |
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| 520 | |a Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. | ||
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10.1007/s00340-010-4341-y doi (DE-627)OLC2074302894 (DE-He213)s00340-010-4341-y-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Hubschmid, W. verfasserin aut Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ 2010 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2010 Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume Bombach, R. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 103(2010), 4 vom: 17. Dez., Seite 933-939 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:103 year:2010 number:4 day:17 month:12 pages:933-939 https://doi.org/10.1007/s00340-010-4341-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_2021 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 103 2010 4 17 12 933-939 |
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10.1007/s00340-010-4341-y doi (DE-627)OLC2074302894 (DE-He213)s00340-010-4341-y-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Hubschmid, W. verfasserin aut Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ 2010 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2010 Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume Bombach, R. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 103(2010), 4 vom: 17. Dez., Seite 933-939 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:103 year:2010 number:4 day:17 month:12 pages:933-939 https://doi.org/10.1007/s00340-010-4341-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_2021 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 103 2010 4 17 12 933-939 |
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10.1007/s00340-010-4341-y doi (DE-627)OLC2074302894 (DE-He213)s00340-010-4341-y-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Hubschmid, W. verfasserin aut Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ 2010 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2010 Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume Bombach, R. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 103(2010), 4 vom: 17. Dez., Seite 933-939 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:103 year:2010 number:4 day:17 month:12 pages:933-939 https://doi.org/10.1007/s00340-010-4341-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_2021 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 103 2010 4 17 12 933-939 |
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10.1007/s00340-010-4341-y doi (DE-627)OLC2074302894 (DE-He213)s00340-010-4341-y-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Hubschmid, W. verfasserin aut Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ 2010 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2010 Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume Bombach, R. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 103(2010), 4 vom: 17. Dez., Seite 933-939 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:103 year:2010 number:4 day:17 month:12 pages:933-939 https://doi.org/10.1007/s00340-010-4341-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_2021 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 103 2010 4 17 12 933-939 |
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10.1007/s00340-010-4341-y doi (DE-627)OLC2074302894 (DE-He213)s00340-010-4341-y-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Hubschmid, W. verfasserin aut Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ 2010 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2010 Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume Bombach, R. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 103(2010), 4 vom: 17. Dez., Seite 933-939 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:103 year:2010 number:4 day:17 month:12 pages:933-939 https://doi.org/10.1007/s00340-010-4341-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_2021 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 103 2010 4 17 12 933-939 |
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530 620 VZ 530 VZ UA 9001 VZ rvk Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ Sound Velocity Sound Wave Bulk Viscosity Sound Absorption Observation Volume |
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Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ |
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Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ |
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Hubschmid, W. |
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electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ h_{2} $ |
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Electrostrictive laser-induced gratings for time-resolved observation of translational-rotational energy transfer in $ H_{2} $ |
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Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. © Springer-Verlag 2010 |
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Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. © Springer-Verlag 2010 |
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Abstract Electrostrictive laser-induced gratings (LIG) have been formed in $ H_{2} $ of various pressures (0.5…5 bar) and with frequencies of the Brillouin modes (sound waves) of about 14 MHz. Under these conditions, the rotational degrees of freedom can only partially follow the temperature variation from the acoustic oscillation. A model is given, which completes the linearized fluid dynamical equations with equations for the rotational state relaxation, separately for the average relaxation of the states for Ortho-$ H_{2} $ and Para-$ H_{2} $. Using such a model, the dispersion of sound frequency is reproduced with an accuracy of a few percent. However, the total dissipation of sound and the observed strong alternation in peak heights in the temporal evolution of the LIG intensity is only approximately predicted by the model. © Springer-Verlag 2010 |
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