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Volumn 17, Issue 5, 2010, Pages

Plastic ablator ignition capsule design for the National Ignition Facility

Author keywords

[No Author keywords available]

Indexed keywords

ABLATORS; CURRENT SIMULATION; DESIGN OPTIMIZATION; FUSION IGNITION; HIGH-DENSITY; IGNITION CAPSULES; IGNITION PROBABILITY; LASER ENERGIES; NATIONAL IGNITION FACILITY; ONE-DIMENSIONAL SIMULATIONS; RAYLEIGH-TAYLOR GROWTH; STATISTICAL BEHAVIOR; TARGET DESIGN; TWO-DIMENSIONAL SIMULATIONS;

EID: 77953002974     PISSN: 1070664X     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3403293     Document Type: Conference Paper
Times cited : (93)

References (26)
  • 1
    • 11144334175 scopus 로고    scopus 로고
    • The National Ignition Facility: Enabling fusion ignition for the 21st century
    • DOI 10.1088/0029-5515/44/12/S14, PII S002955150488517X, Inertial Fusion Statae of the Art-A Collection of overview and Technical Papers from IFSA2003
    • G. H. Miller, E. I. Moses, and C. R. Wuest, Nucl. Fusion NUFUAU 0029-5515 44, S228 (2004). 10.1088/0029-5515/44/12/S14 (Pubitemid 40026156)
    • (2004) Nuclear Fusion , vol.44 , Issue.12
    • Miller, G.H.1    Moses, E.I.2    Wuest, C.R.3
  • 12
    • 77952967357 scopus 로고    scopus 로고
    • private communication
    • H. Huang, private communication (2009).
    • (2009)
    • Huang, H.1
  • 17
    • 77953010569 scopus 로고    scopus 로고
    • private communication
    • J. D. Salmonson, private communication (2007).
    • (2007)
    • Salmonson, J.D.1
  • 18
    • 77952968240 scopus 로고    scopus 로고
    • note
    • moutside = (90.0/ 2.3) + { 0.20/ [(/70.0) 0.6 + (/1200.0) 3.5] }. For modes 12, corrections are made individually to the amplitudes to agree with measured surfaces. These 3D surface coefficients are then converted to 2D coefficients by multiplying each by the square root of the number of m -modes that would contribute in 3D, R 2D =± 2+1 Rm, where the sign of the coefficient is chosen randomly for each mode. For the four internal dopant layers, the spectral coefficients are assumed to be one-fifth of the power of the outer ablator surface and the surface perturbations to add successively until the last dopant surface is defined. Note that this prescription applies for modes =1-30. For higher modes, a more complicated prescription is required which progressively decorrelates the outer surface from inner surfaces with increasing mode number.
  • 24
    • 44649165284 scopus 로고    scopus 로고
    • BAPSA6 0003-0503 ()
    • J. D. Salmonson, Bull. Am. Phys. Soc. BAPSA6 0003-0503 52 (16), 273 (2007).
    • (2007) Bull. Am. Phys. Soc. , vol.52 , Issue.16 , pp. 273
    • Salmonson, J.D.1
  • 25
    • 77953004029 scopus 로고    scopus 로고
    • The intuitive sense of margin M is better captured by defining it as MApproaches the limitITF-1. By this definition, margin measures the distance from the ignition cliff in units of ITF. At the ignition cliff, where ITF1, M=0 and there is then no "margin. 201d
    • The intuitive sense of margin M is better captured by defining it as MApproaches the limitITF-1. By this definition, margin measures the distance from the ignition cliff in units of ITF. At the ignition cliff, where ITF1, M=0 and there is then no "margin."
  • 26
    • 44649141821 scopus 로고    scopus 로고
    • Robustness studies of ignition targets for the National Ignition Facility in two dimensions
    • DOI 10.1063/1.2890123
    • D. S. Clark, S. W. Haan, and J. D. Salmonson, Phys. Plasmas PHPAEN 1070-664X 15, 056305 (2008). 10.1063/1.2890123 (Pubitemid 351776756)
    • (2008) Physics of Plasmas , vol.15 , Issue.5 , pp. 056305
    • Clark, D.S.1    Haan, S.W.2    Salmonson, J.D.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.