Titlebook: Integration of Mitochondrial Function; John J. Lemasters,Charles R. Hackenbrock,Hans V. W Book 1988 Springer Science+Business Media New Yo

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書目名稱Integration of Mitochondrial Function影響因子(影響力)




書目名稱Integration of Mitochondrial Function影響因子(影響力)學(xué)科排名




書目名稱Integration of Mitochondrial Function網(wǎng)絡(luò)公開(kāi)度




書目名稱Integration of Mitochondrial Function網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書目名稱Integration of Mitochondrial Function被引頻次




書目名稱Integration of Mitochondrial Function被引頻次學(xué)科排名




書目名稱Integration of Mitochondrial Function年度引用




書目名稱Integration of Mitochondrial Function年度引用學(xué)科排名




書目名稱Integration of Mitochondrial Function讀者反饋




書目名稱Integration of Mitochondrial Function讀者反饋學(xué)科排名

低能兒

The initial shock pressures were 13 kbar and 17 kbar after ps-pulses with an energy of 50 .J and 1 mJ, respectively, 24 kbar after a 1 mJ ns-pulse, and 71 kbar after a 10 mJ ns-pulse. After formation of the shock front, the shock pressure decayed approximately proportional to 1/... The maximum expan

用樹(shù)皮

Measured

大量殺死

S. Ferguson-Miller,K. Rajarathnam,J. Hochman,M. Schindlert flow regimes often associated with bubbly flows. The symposium attracts wide and extensive interest from engineers, physical, chemical, biological and medical scientists and applied mathematicians. The sci- entific committee sought to achieve a balance between theory and experiment over a range of

SCORE

G. Lenaz,R. Fato,C. Castelluccio,M. Degli Esposti,C. M. Samworth,M. Battino,G. Parenti Castelliont takes a classical smooth form (approximately 100 m wide). In the second case, the decompression wave structure and the melt state behind the saturation front turn out to be principally different. The jumps in the mass velocity and viscosity practically left out the pressure inside the cavitation

商議

Brad Chazotte,Charles R. Hackenbrockont takes a classical smooth form (approximately 100 m wide). In the second case, the decompression wave structure and the melt state behind the saturation front turn out to be principally different. The jumps in the mass velocity and viscosity practically left out the pressure inside the cavitation

按等級(jí)

W. Marshall Anderson,Deborah L. Delinck-Gordonof the medium. The widths of the shock waves reach values in the range of tens of nano seconds to beyond 100 ns. The simultaneously generated breakdown bubble gets about half of the energy of the shock wave. Bubble energy rises linearly with the laser pulse energy with different slopes depending on

極為憤怒

Jo A. Freedman,Samuel H. P. Chan,P. Nichollsfor both the collapse of a single cavitation bubble and the impact of flow on the collapse are reviewed and results for simulations of shock propagation in a domain containing several bubbles are then presented. We conclude by discussing possible future studies and the outlook for DNS of cavitating

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