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UDC:  534.16: 535.341            https://doi.org/10.62965/tnu.sns.2024.1.6                 Download article

 

Khodjaev Y.P., Salikhov T.Kh. Sulaimonov A. E., Mahmalatif A.

Scientific Research Institute of Tajik National University

 

Based on the system of nonlinear heat conduction  equations, which takes into account the relaxation of the heat flux for the gas layer, the sample, and the substrate, a system of equations is obtained for temperature fluctuations at the fundamental harmonic (FH) of a nonlinear photoacoustic (PA) signal.

It is believed that all three layers in the PA-chamber have their own relaxation times, and the irradiated photon flux is modulated according to the harmonic law. The temperature dependence of thermophysical and optical parameters is represented by thermal coefficients. By solving the boundary problem, general expressions were obtained for the oscillatory component of the temperature perturbation in the exhaust gas, and then, according to a well-known scheme, for pressure fluctuations in the gas layer. The obtained expressions are analyzed.

The frequency dependence of the amplitude and phase of this signal is numerically calculated for two possible substrates: the substrate is a thermal insulator and the substrate is an ideal conductor. It has been established that the frequency dependence of the PA-signal amplitude for these cases is antiphase. While, this dependence for the phase of the PA-signal is consistent in phases moreover, the values of the maximum and minimum coincide. The only significant difference is that in the region of zero modulation frequencies, the phase of the signal for a substrate made of a thermal insulator is positive, while for a substrate made of an ideal conductor is negative.

 

Key words: optoacoustic, heat flow, heat flow relaxation, thermal nonlinearity, photoacoustic, nonlinear photoacoustic response, fundamental harmonic, gas microphone registration.

 

Information about the authors

 

Salikhov Tagaymurod  Haitovich – Scientific Research Institute of Tajik National University, 

doctor of physical and mathematical sciences, professor, the chief researcher of Department of "Physics of the Condensed Matter".

Address: 734025, Dushanbe, Rudaki, Avenue 17. Phone: (+992) 919-24-83-11.

Е-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.

 

Yunus Khodjaev  Pardalievich - Scientific Research Institute of Tajik National University,

Ph.D., Leading Researcher, Department of Condensed Matter Physics. Address: 734025, Republic of Tajikistan, Dushanbe, Rudaki Avenue, 17.

Phone: 918-24-03-50.

E-mail: kh.yunus84@mail.ru

 

Sulaimonov Aidar Eronshoevich – Scientific Research Institute of Tajik National University,

Researcher  of the Department of Condensed Matter Physics.

Address: 734025, Republic of Tajikistan, Dushanbe, Rudaki Avenue, 17.

Phone: 931923312.

E-mail:  This email address is being protected from spambots. You need JavaScript enabled to view it.

 

Alisher Makhmalatif – Scientific Research Institute of Tajik National University,

Ph.D, Senior Researcher of the Condensed Matter Physics Department, Research Institute of the Tajik National University.

Аddress: 734025, Republic of Tajikistan, Dushanbe, Rudaki Avenue 17.

Phone: 935−93−19−31,

E−mail: This email address is being protected from spambots. You need JavaScript enabled to view it.

 

REVIEWER: Makhsudov B.I., Doctor physical and mathematical sciences, Professor

 

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Article received: 12.09.2023

Approved after review: 11.10.2023

Accepted for publication: 20.11.2023

 

   
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