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Evolution of Waveforms During Propagation in Solids. / Khantuleva, Tatiana Aleksandrovna .

Mathematical Modeling of Shock-Wave Processes in Condensed Matter: From Statistical Thermodynamics to Control Theory. Singapore : Springer Nature, 2022. p. 251-281 (Shock Wave and High Pressure Phenomena).

Research output: Chapter in Book/Report/Conference proceedingChapterResearchpeer-review

Harvard

Khantuleva, TA 2022, Evolution of Waveforms During Propagation in Solids. in Mathematical Modeling of Shock-Wave Processes in Condensed Matter: From Statistical Thermodynamics to Control Theory. Shock Wave and High Pressure Phenomena, Springer Nature, Singapore, pp. 251-281.

APA

Khantuleva, T. A. (2022). Evolution of Waveforms During Propagation in Solids. In Mathematical Modeling of Shock-Wave Processes in Condensed Matter: From Statistical Thermodynamics to Control Theory (pp. 251-281). (Shock Wave and High Pressure Phenomena). Springer Nature.

Vancouver

Khantuleva TA. Evolution of Waveforms During Propagation in Solids. In Mathematical Modeling of Shock-Wave Processes in Condensed Matter: From Statistical Thermodynamics to Control Theory. Singapore: Springer Nature. 2022. p. 251-281. (Shock Wave and High Pressure Phenomena).

Author

Khantuleva, Tatiana Aleksandrovna . / Evolution of Waveforms During Propagation in Solids. Mathematical Modeling of Shock-Wave Processes in Condensed Matter: From Statistical Thermodynamics to Control Theory. Singapore : Springer Nature, 2022. pp. 251-281 (Shock Wave and High Pressure Phenomena).

BibTeX

@inbook{4abbd9b924974f67a22b4b771ecf3515,
title = "Evolution of Waveforms During Propagation in Solids",
abstract = "In Chapter 7 we have obtained the explicit solution to the problem of the shock-induced waveforms propagation that allows us to describe the medium response both during the loading and post-shock effects. As experiments show [1], the model parameters depending on the distance travelled by the wave after impact evolve during the waveform propagation along the material. In the section 7.10 we have already traced the evolution of the parameters by using their experimental values obtained for the waveforms recorded at various distances from the impact surface (see Fig. 7.11). It is found out that all experimental points obtained by using the waveforms measured at different traveled distances fall down on the straight lines going at different angles for each material. In Chapter 8, the integral model developed in Chapter 7 is applied to describe the shock-induced waveform evolution during its propagation inside the material through the evolution of the model parameters by methods developed in cybernetic physics and considered in Chapter 6. The goal function for the waveform evolution is determined by maximum of the total entropy production that pointes out the direction of the system evolution in accordance with MEP [2]. The speed gradient (SG) algorithm determines the fastest evolutionary paths to the goal. Comparison of the theoretical paths obtained in this way with the experimental results for quasi-stationary regime of the waveform propagation shows good agreement between them.The parameters used in the integral model of the waveform, as it was found out, determine two limiting states inside the waveform. The observed decrease in the parameter during the so-called elastic precursor relaxation makes the material state less solid while the parameter defines the time interval needed for the restoration (at least partial) of the solid material state when the so-called plastic front reaches the plateau of the compression pulse. It means that the parameters evolve inside the waveform whereas the waveform evolution at rather large distance from the impact surface is adequately described by the integral model with the constant parameters over the waveform duration.The described structure evolution inside the finite-duration waveform is an example of a process in which, as a result of the self-organization of new mesoscopic structures, the generalized integral entropy production after the unloading front can become negative.",
keywords = "shock-induced waveform, stress relaxation, temporal evolution, Speed Gradient principle, integral entropy production",
author = "Khantuleva, {Tatiana Aleksandrovna}",
note = "Bibliographic Information • Book Title Mathematical Modeling of Shock-Wave Processes in Condensed Matter • Book Subtitle From Statistical Thermodynamics to Control Theory • Authors Tatiana Aleksandrovna Khantuleva • Series Title Shock Wave and High Pressure Phenomena • DOI https://doi.org/10.1007/978-981-19-2404-0 • Publisher Springer Singapore • eBook Packages Physics and Astronomy, Physics and Astronomy (R0) • Copyright Information The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Nature Singapore Pte Ltd. 2022 • Hardcover ISBN 978-981-19-2403-3 • eBook ISBN 978-981-19-2404-0 • Series ISSN 2197-9529 • Series E-ISSN 2197-9537 • Edition Number1 • Number of Pages XV, 336 • Number of Illustrations 19 b/w illustrations, 58 illustrations in colour • Topics Statistical Physics, Classical and Continuum Physics, Condensed Matter, Solid Mechanics ",
year = "2022",
month = jul,
day = "19",
language = "English",
isbn = "978-981-19-2403-3",
series = "Shock Wave and High Pressure Phenomena",
publisher = "Springer Nature",
pages = "251--281",
booktitle = "Mathematical Modeling of Shock-Wave Processes in Condensed Matter",
address = "Germany",

}

RIS

TY - CHAP

T1 - Evolution of Waveforms During Propagation in Solids

AU - Khantuleva, Tatiana Aleksandrovna

N1 - Bibliographic Information • Book Title Mathematical Modeling of Shock-Wave Processes in Condensed Matter • Book Subtitle From Statistical Thermodynamics to Control Theory • Authors Tatiana Aleksandrovna Khantuleva • Series Title Shock Wave and High Pressure Phenomena • DOI https://doi.org/10.1007/978-981-19-2404-0 • Publisher Springer Singapore • eBook Packages Physics and Astronomy, Physics and Astronomy (R0) • Copyright Information The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Nature Singapore Pte Ltd. 2022 • Hardcover ISBN 978-981-19-2403-3 • eBook ISBN 978-981-19-2404-0 • Series ISSN 2197-9529 • Series E-ISSN 2197-9537 • Edition Number1 • Number of Pages XV, 336 • Number of Illustrations 19 b/w illustrations, 58 illustrations in colour • Topics Statistical Physics, Classical and Continuum Physics, Condensed Matter, Solid Mechanics

PY - 2022/7/19

Y1 - 2022/7/19

N2 - In Chapter 7 we have obtained the explicit solution to the problem of the shock-induced waveforms propagation that allows us to describe the medium response both during the loading and post-shock effects. As experiments show [1], the model parameters depending on the distance travelled by the wave after impact evolve during the waveform propagation along the material. In the section 7.10 we have already traced the evolution of the parameters by using their experimental values obtained for the waveforms recorded at various distances from the impact surface (see Fig. 7.11). It is found out that all experimental points obtained by using the waveforms measured at different traveled distances fall down on the straight lines going at different angles for each material. In Chapter 8, the integral model developed in Chapter 7 is applied to describe the shock-induced waveform evolution during its propagation inside the material through the evolution of the model parameters by methods developed in cybernetic physics and considered in Chapter 6. The goal function for the waveform evolution is determined by maximum of the total entropy production that pointes out the direction of the system evolution in accordance with MEP [2]. The speed gradient (SG) algorithm determines the fastest evolutionary paths to the goal. Comparison of the theoretical paths obtained in this way with the experimental results for quasi-stationary regime of the waveform propagation shows good agreement between them.The parameters used in the integral model of the waveform, as it was found out, determine two limiting states inside the waveform. The observed decrease in the parameter during the so-called elastic precursor relaxation makes the material state less solid while the parameter defines the time interval needed for the restoration (at least partial) of the solid material state when the so-called plastic front reaches the plateau of the compression pulse. It means that the parameters evolve inside the waveform whereas the waveform evolution at rather large distance from the impact surface is adequately described by the integral model with the constant parameters over the waveform duration.The described structure evolution inside the finite-duration waveform is an example of a process in which, as a result of the self-organization of new mesoscopic structures, the generalized integral entropy production after the unloading front can become negative.

AB - In Chapter 7 we have obtained the explicit solution to the problem of the shock-induced waveforms propagation that allows us to describe the medium response both during the loading and post-shock effects. As experiments show [1], the model parameters depending on the distance travelled by the wave after impact evolve during the waveform propagation along the material. In the section 7.10 we have already traced the evolution of the parameters by using their experimental values obtained for the waveforms recorded at various distances from the impact surface (see Fig. 7.11). It is found out that all experimental points obtained by using the waveforms measured at different traveled distances fall down on the straight lines going at different angles for each material. In Chapter 8, the integral model developed in Chapter 7 is applied to describe the shock-induced waveform evolution during its propagation inside the material through the evolution of the model parameters by methods developed in cybernetic physics and considered in Chapter 6. The goal function for the waveform evolution is determined by maximum of the total entropy production that pointes out the direction of the system evolution in accordance with MEP [2]. The speed gradient (SG) algorithm determines the fastest evolutionary paths to the goal. Comparison of the theoretical paths obtained in this way with the experimental results for quasi-stationary regime of the waveform propagation shows good agreement between them.The parameters used in the integral model of the waveform, as it was found out, determine two limiting states inside the waveform. The observed decrease in the parameter during the so-called elastic precursor relaxation makes the material state less solid while the parameter defines the time interval needed for the restoration (at least partial) of the solid material state when the so-called plastic front reaches the plateau of the compression pulse. It means that the parameters evolve inside the waveform whereas the waveform evolution at rather large distance from the impact surface is adequately described by the integral model with the constant parameters over the waveform duration.The described structure evolution inside the finite-duration waveform is an example of a process in which, as a result of the self-organization of new mesoscopic structures, the generalized integral entropy production after the unloading front can become negative.

KW - shock-induced waveform, stress relaxation, temporal evolution, Speed Gradient principle, integral entropy production

UR - https://link.springer.com/chapter/10.1007/978-981-19-2404-0_8

M3 - Chapter

SN - 978-981-19-2403-3

T3 - Shock Wave and High Pressure Phenomena

SP - 251

EP - 281

BT - Mathematical Modeling of Shock-Wave Processes in Condensed Matter

PB - Springer Nature

CY - Singapore

ER -

ID: 98857929