Researching | Laser driven dynamic compression of materials

Journals >High Power Laser and Particle Beams >Volume 34 >Issue 1 >Page 011001 > Article

High Power Laser and Particle Beams
Vol. 34, Issue 1, 011001 (2022)

Laser driven dynamic compression of materials

Mu Li¹, Hongping Zhang², Shi Chen¹, Peidong Tao^1,3..., Hang Zhu¹, Cangtao Zhou¹, Jianheng Zhao⁴ and Chengwei Sun^5,6|Show fewer author(s)

Author Affiliations

¹Shenzhen Key Laboratory of Ultra-intense Laser and Advanced Material Technology, Center for Advanced Material Diagnostic Technology, College of Engineering Physics, Shenzhen Technology University, Shenzhen 518118, China

²Big Data and Internet College, Shenzhen Technology University, Shenzhen 518118, China

³College of Physics, Sichuan University, Chengdu 610065, China

⁴Institute of Applied Electronics, CAEP, Mianyang 621900, China

⁵Institute of Fluid Physics, CAEP, Mianyang 621900, China

⁶Shanghai Institute of Laser Plasma, CAEP, Shanghai 201800, China

show less

DOI: 10.11884/HPLPB202234.210357 Cite this Article

Mu Li, Hongping Zhang, Shi Chen, Peidong Tao, Hang Zhu, Cangtao Zhou, Jianheng Zhao, Chengwei Sun. Laser driven dynamic compression of materials[J]. High Power Laser and Particle Beams, 2022, 34(1): 011001 Copy Citation Text

show less

Abstract

Laser driven dynamic compression experiments play the central role in extreme pressure and density research, and are important to a number of fields, including planetary geophysics, material science, and inertial confinement fusion, benefit to improve understandings of properties of materials at extreme conditions and their applications. Recently laser driven compression techniques have been developing quickly together with laser facility, laser plasma interaction, target fabrication and diagnostic techniques. On contrast to other loading platform, it is good at ramp compression, decaying shock compression and complex loading path, and allows micro-scale probe combined with macro-scale measurements, ultra-high pressure and strain rate. This review summarizes this technique from the aspects of thermodynamics of compression, laser drive mechanism, laser drive experimental techniques and recent advances of extreme compression of materials.

Keywords

dynamic high pressure extreme conditions laser dive planetary science properties of material

$ \dot{m}\cong 143{I}_{}^{1/3}{\left({\lambda }_{\mathrm{l}}\right)}^{-4/3} $

(1)

View in Article

$ p\cong \left(8～9\right){I}_{}^{2/3}{{(\lambda }_{\mathrm{l}})}^{-\tfrac{2}{3}} $

(2)

View in Article

$ p\cong (11\pm 0.02){I}_{}^{0.71\pm 0.01} $

(3)

View in Article

$ p\cong 13{I}_{}^{0.75} $

(4)

View in Article

$ \eta {P}_{\mathrm{l}\mathrm{a}\mathrm{s}\mathrm{e}\mathrm{r}}=4.4{A}_{\mathrm{W}}{T}_{\mathrm{r}}^{3.3}+6.25{A}_{\mathrm{h}}{T}_{\mathrm{r}}^{4} $

(5)

View in Article

$ p=3{T}_{\mathrm{r}}^{3.5} $

(6)

View in Article

$ {U}_{\mathrm{s}}={c}_{0}+\mathrm{ }\mathrm{ }\mathrm{ }\mathrm{ }\mathrm{s}{u}_{{\rm{p}}}=\frac{{c}_{0}}{1-s\eta } $

(7)

View in Article

$ {u}_{{\rm{p}}}=\frac{\eta {c}_{0}}{1-s\eta } $

(8)

View in Article

$ \frac{{V}_{{\rm{H}}}}{{V}_{0}}=\frac{{U}_{{\rm{s}}}-{u}_{{\rm{p}}}}{{U}_{{\rm{s}}}}=\frac{s-1+{c}_{0}/{U}_{{\rm{s}}}}{s}=1-\eta $

(9)

View in Article

$ {P}_{{\rm{H}}}-{P}_{0}=\frac{{U}_{{\rm{s}}}{u}_{{\rm{p}}}}{{V}_{0}}=\frac{{U}_{{\rm{s}}}\left({U}_{{\rm{s}}}-{c}_{0}\right)}{s{V}_{0}}=\frac{{c}_{0}^{2}\eta }{{V}_{0}{\left(1-s\eta \right)}^{2}} $

(10)

View in Article

$ {E}_{{\rm{H}}}-{E}_{0}=\left({P}_{{\rm{H}}}+{P}_{0}\right)\left({V}_{0}-{V}_{{\rm{H}}}\right)/2=\frac{{\left({U}_{{\rm{s}}}-{c}_{0}\right)}^{2}}{2{s}^{2}{V}_{0}} $

(11)

View in Article

$ \mathrm{d}{S}={\left.\frac{\partial {S}}{\partial {T}}\right|}_{V}\mathrm{d}T+{\left.\frac{\partial {S}}{\partial {V}}\right|}_{T}\mathrm{d}V=\frac{{C}_{V}}{T}\mathrm{d}T+\frac{{C}_{V}\gamma }{V}\mathrm{d}V $

(12)

View in Article

$ T{\left.\frac{\mathrm{d}{S}}{\mathrm{d}{V}}\right|}_{\mathrm{H}}={\left.\frac{\mathrm{d}{E}}{\mathrm{d}{V}}\right|}_{{\rm{H}}}+{P}_{{\rm{H}}}=\frac{\mathrm{d}\left[\left({P}_{{\rm{H}}}+{P}_{0}\right)\left({V}_{0}-{V}_{{\rm{H}}}\right)/2\right]}{\mathrm{d}V}+{P}_{{\rm{H}}}=\frac{1}{2}\frac{{\rm{d}}P}{{\rm{d}}V}{\Bigg|}_{{\rm{H}}}\left({V}_{0}-{V}_{{\rm{H}}}\right)+\frac{{P}_{{\rm{H}}}}{2}\equiv f\left(V\right) $

(13)

View in Article

$ \frac{\mathrm{d}{{T}}_{{\rm{H}}}}{\mathrm{d}{V}}+\frac{\gamma }{V}{{T}}_{{\rm{H}}}=f\left(V\right)/{C}_{V} $

(14)

View in Article

$ {T}_{{\rm{H}}}\left({\eta }_{{\rm{H}}}\right){=T}_{0}{{\rm{e}}}^{\int_{0}^{{\eta }_{{\rm{H}}}}\tfrac{\gamma }{1-\eta }{\rm{d}}\eta }-{V}_{0}{{\rm{e}}}^{\int_{0}^{{\eta }_{{\rm{H}}}}\tfrac{\gamma }{1-\eta }{\rm{d}}\eta }\int_{0}^{{\eta }_{{\rm{H}}}}\dfrac{f\left(\eta \right){{\rm{e}}}^{-\int _{0}^{\eta }\tfrac{\gamma }{1-\eta }{\rm{d}}\eta }}{{C}_{V}}{\rm{d}}\eta $

(15)

View in Article

$ \frac{\mathrm{\gamma }}{{\gamma }_{0}}={\left(\frac{V}{{V}_{0}}\right)}^{q} $

(16)

View in Article

$ {T}_{{\rm{H}}}\left({\eta }_{{\rm{H}}}\right){=T}_{0}{{\rm{e}}}^{{\gamma }_{0}{\eta }_{{\rm{H}}}}-{{V}_{0}{\rm{e}}}^{{\gamma }_{0}{\eta }_{{\rm{H}}}}\int_{0}^{{\eta }_{{\rm{H}}}}\dfrac{f\left(\eta \right){{\rm{e}}}^{{-\gamma }_{0}\eta }}{{C}_{V}}{\rm{d}}\eta $

(17)

View in Article

$ {C}_{V{\rm{H}}}=\dfrac{{\left(\dfrac{\partial E}{\partial V}\right)}_{{\rm{H}}}+{P}_{{\rm{H}}}}{{\left(\dfrac{\partial T}{\partial V}\right)}_{{\rm{H}}}+\dfrac{\gamma {T}_{{\rm{H}}}}{V}}=\dfrac{{\left({U}_{{\rm{s}}}-{c}_{0}\right)}^{2}\left[{U}_{{\rm{s}}}\left(s-1\right)+{c}_{0}\right]}{{s}^{2}\left\{\left[{{U}_{{\rm{s}}}}^{2}\left(s-1\right)+{c}_{0}{U}_{{\rm{s}}}\right]\dfrac{\partial {T}_{{\rm{H}}}}{\partial {U}_{{\rm{s}}}}-{\gamma c}_{0}{T}_{{\rm{H}}}\right\}}={\left.\dfrac{{\left({U}_{{\rm{s}}}-{c}_{0}\right)}^{2}}{{s}^{2}{U}_{{\rm{s}}}\left(\dfrac{\partial {T}_{{\rm{H}}}}{\partial {U}_{{\rm{s}}}}-\dfrac{{{\gamma }_{0}c}_{0}}{s{{U}_{{\rm{s}}}}^{2}}{T}_{{\rm{H}}}\right)}\right|}_{q=1} $

(18)

View in Article

$ {\mathrm{\gamma }}_{\mathrm{H}}=\dfrac{2\left({c}_{{\rm{b}}{\rm{H}}}^{2}+{\left.\dfrac{\partial P}{\partial V}\right|}_{{\rm{H}}}{V}_{{\rm{H}}}\right)}{{V}_{{\rm{H}}}\left[{P}_{{\rm{H}}}+{\left.\dfrac{\partial P}{\partial V}\right|}_{{\rm{H}}}\left({V}_{0}{-V}_{{\rm{H}}}\right)\right]} $

(19)

View in Article

$ {\sigma }_{{\rm{R}}}\left({U}_{{\rm{p}}1}\right)={p}_{{\rm{R}}}+\frac{2}{3}Y={\rho }_{0}{\int }_{0}^{{U}_{{\rm{p}}1}}{C}_{{\rm{L}}}\left({U}_{{\rm{p}}}\right){\rm{d}}{U}_{{\rm{p}}} $

(20)

View in Article

$ {V}_{{\rm{R}}}\left({U}_{{\rm{p}}1}\right)={V}_{0}-{V}_{0}{\int }_{0}^{{U}_{{\rm{p}}1}}\frac{{\rm{d}}{U}_{{\rm{p}}}}{{C}_{{\rm{L}}}\left({U}_{{\rm{p}}}\right)} $

(21)

View in Article

$ \mathrm{d}{S}={\left.\frac{\partial {S}}{\partial {T}}\right|}_{V}\mathrm{d}T+{\left.\frac{\partial {S}}{\partial {V}}\right|}_{T}\mathrm{d}V=\frac{{C}_{V}}{T}\mathrm{d}T+\frac{{C}_{V}\gamma }{V}\mathrm{d}V $

(22)

View in Article

$ {T}{\left.\frac{\mathrm{d}{S}}{\mathrm{d}{V}}\right|}_{{\rm{R}}}={\left.\frac{\mathrm{d}{E}}{\mathrm{d}{V}}\right|}_{{\rm{R}}}+{P}_{{\rm{R}}}\equiv {f}_{{\rm{R}}}\left(V\right) $

(23)

View in Article

$ \frac{\mathrm{d}{{T}}_{{\rm{R}}}}{\mathrm{d}{V}}+\frac{\gamma }{V}{{T}}_{{\rm{R}}}={f}_{{\rm{R}}}\left(V\right)/{C}_{V} $

(24)

View in Article

$ \frac{{T}\mathrm{d}{S}}{{\rm{d}}V}\equiv {f}_{{\rm{R}}}\left(V\right)\approx -\mathrm{\omega }\frac{2}{3}Y $

(25)

View in Article

$ {T}_{1}{={T}_{\mathrm{R}}\left({\eta }_{1}\right)=T}_{0}{\mathrm{e}}^{\int_{0}^{{{\eta }_{1}}}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }-{V}_{0}{\mathrm{e}}^{\int _{0}^{{{\eta }_{1}}}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }\int_{0}^{{{\eta }_{1}}}\dfrac{f\left(\eta \right){{\rm{e}}}^{-\int_{0}^{{\eta }}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }}{{C}_{V}}\mathrm{d}\eta $

(26)

View in Article

$ {\left.{P}_{\mathrm{R}}\left({\eta }_{1}\right)-{P}_{\mathrm{s}}\left({\eta }_{1}\right)=\frac{\partial P}{\partial T}\right|}_{V}\left({T}_{\mathrm{R}}-{T}_{\mathrm{s}}\right)={\left.\frac{\gamma {C}_{V}}{{V}_{1}}\right|}_{V}\left({T}_{\mathrm{R}}-{T}_{\mathrm{s}}\right) =-3\alpha {K}_{\mathrm{T}}{V}_{0}{\mathrm{e}}^{\int_{0}^{{{\eta }_{1}}}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }\int_{0}^{{{\eta }_{1}}}\dfrac{f\left(\eta \right){\mathrm{e}}^{-\int_{0}^{{\eta }}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }}{{C}_{V}}\mathrm{d}\eta $

(27)

View in Article

$ Y\left(V\right)=\frac{3}{2}[\sigma _{\mathrm{R}}\left(V\right)-p_{\mathrm{R}}\left(V\right)] $

(28)

View in Article

$ {E}_{\mathrm{R}}\left({V}_{1}\right)=-{\int }_{{V}_{0}}^{{V}_{\mathrm{e}\mathrm{p}}}\sigma \mathrm{d}V-\int_{{V}_{\mathrm{e}\mathrm{p}}}^{{{V}_{1}}}\left[\left(-3\alpha {K}_{\mathrm{T}}{V}_{0}{\mathrm{e}}^{\int_{0}^{{{\eta }_{1}}}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }\int_{0}^{{{\eta }_{1}}}\dfrac{f\left(\eta \right){\mathrm{e}}^{-\int_{0}^{{\eta }}\tfrac{\gamma }{1-\eta }\mathrm{d}\eta }}{{C}_{V}}\mathrm{d}\eta \right)+\omega \dfrac{2}{3}Y\right]\mathrm{d}V $

(29)

View in Article

$ I\left(\lambda ,T\right)={\varepsilon }_{\lambda } \frac{2h{c}^{2}}{{\lambda }^{5}}\frac{1}{-1+{{\rm{e}}}^{hc/\lambda kT}}\text{} $

(30)

View in Article

$ P\left(X\right)=3{K}_{0,T}\left(1-X\right){X}^{-2}{{\rm{e}}}^{\left[1.5\left({K'}_{0,T}-1\right)\left(1-X\right)\right]} $

(31)

View in Article

Get PDF(in Chinese)

Figures&Tables (18)

References (117)

Copy Citation Text

Mu Li, Hongping Zhang, Shi Chen, Peidong Tao, Hang Zhu, Cangtao Zhou, Jianheng Zhao, Chengwei Sun. Laser driven dynamic compression of materials[J]. High Power Laser and Particle Beams, 2022, 34(1): 011001

Download Citation

Save the article for my favorites

Paper Information

Recommended Topics

laser devices and laser physics

Lasers and Laser Optics

laser manufacturing

Instrumentation, Measurement and Metrology

Set citation alerts for the article

Please enter your email address