Etant donné labrì eveté des phénomènes rencontrés, il n'est pas possible d'effectuer la mesure de la température de manì ere directe avec par exemple un thermocouple. La seule possibilité s'offrant aux expériences de compression dynamique est la mesure de l'´ emission propre Dans le cas de matériaux transparents en aval du front de choc (eau, plexiglass...), la luminosité du front de choc permet de remonteràremonterà sa température Dans le cas d'un matériau opaque comme le fer, la situation devient naturellement plus compliquée Ou pourrait alors imaginer une mesure de l'´ emission propre ayant lieu pendant l'intervalle de temps o` u le choc traverse l'´ epaisseur de peau juste avant le débouché. L'´ epaisseur de peau d'un métaí etant de quelques 0,1 µm et la vitesse d'un choc de ?10 km/s, le temps de transit serait de l'ordre de 10 ps, ce qui nécessite une résolution instrumentale de l'ordre de la ps. Bien que la technologie actuelle réponderépondè a de telles exigences, Zel'dovich & Raizer [1967] nous rappellent que le front de choc devraitêtredevraitêtreparalì elè a la surface librè a moins de 10 nm près, ce quì a l'heure actuelle est impossiblè a réaliser, Une mesure de température peut alorsêtrealorsêtre effectuéederrì ere l'onde de raréfaction qui remonte dans la cible comprimée après le débouché du choc. Nous avons vu dans (2.4.3) que dans le cas o` u la surface est libre C'est pourquoi dans ce chapitre nous exploitons la configuration de cible Fe/LiF pour effectuer une mesure de la température du fer en détente partielle dans le LiF ,
´ emission propre effectuant une mesure de la luminosité de l'interface Fe/LiF au cours du temps. Dans (6.1), nous estimons le transfert thermique dans la fenêtre de LiF et le transfert radiatif dans l'´ epaisseur de peau du fer en détente. Ces effets s'avèrentavèrentêtre négligeables et la température de brillance peut ainsî etre associéè a la température d'interface, nous accédonsaccédonsà la températuré equivalente de corps ,
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