Takuya Matsuda - Academia.edu (original) (raw)
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Papers by Takuya Matsuda
Progress of Theoretical and Experimental Physics, Apr 1, 1973
arXiv (Cornell University), Feb 6, 2004
arXiv (Cornell University), Feb 10, 2004
arXiv (Cornell University), Oct 9, 2001
arXiv (Cornell University), Oct 9, 2001
Progress of theoretical and experimental physics, Nov 1, 2015
arXiv (Cornell University), May 28, 1998
Astrophysics and space science library, 1999
Progress of Theoretical and Experimental Physics, Jun 1, 1970
Progress of Theoretical and Experimental Physics, 1979
Progress of Theoretical and Experimental Physics, Oct 1, 2001
Monthly Notices of the Royal Astronomical Society, Mar 1, 2000
Monthly Notices of the Royal Astronomical Society, Dec 1, 1987
Monthly Notices of the Royal Astronomical Society, Jun 1, 1987
Progress of Theoretical and Experimental Physics, 2015
The time-steady equation for a 1D wind accretion flow, i.e. the Bondi-Hoyle-Lyttleton (BHL) equat... more The time-steady equation for a 1D wind accretion flow, i.e. the Bondi-Hoyle-Lyttleton (BHL) equation, is investigated analytically. The BHL equation is well known to have infinitely many solutions. Traditionally, the accretion radius has been assumed to be 2GM/v 2 ∞ , but its mathematical foundation has not been clarified because of the non-uniqueness of the solution. Here, we assume that the solution curves possess physically nice characteristics, i.e. velocity and line mass-density increase monotonically with radial distance. This condition restricts the accretion radius to the range (0.71 − 1.0) × 2GM/v 2 ∞. Further assumptions, specifically, that the solution curves for velocity and line mass-density are convex upward, restrict the accretion radius to (0.84 − 0.94) × 2GM/v 2 ∞ , and 0.90 × 2GM/v 2 ∞ , respectively. Therefore, we conclude that the accretion radius is almost uniquely determined to be 0.90 × 2GM/v 2 ∞ .
On essaie de determiner dans quelle mesure la trainee sur un corps depend de la force gravitation... more On essaie de determiner dans quelle mesure la trainee sur un corps depend de la force gravitationnelle, afin d'evaluer l'echelle de temps correcte de la croissance des planetes
Symposium - International Astronomical Union
The Direct Simulation Monte Carlo (DSMC) method, developed originally to calculate rarefied gas d... more The Direct Simulation Monte Carlo (DSMC) method, developed originally to calculate rarefied gas dynamical problems, is applied to continuous flow including shocks assuming that the Knudsen number is sufficiently small. In particular, we study the formation of spiral shocks in the accretion disc of a close binary system. The method involves viscosity and thermal conduction automatically, and can thus simulate turbulent viscosity.
Monthly Notices of the Royal Astronomical Society
Monthly Notices of the Royal Astronomical Society
Monthly Notices of the Royal Astronomical Society
Progress of Theoretical and Experimental Physics, Apr 1, 1973
arXiv (Cornell University), Feb 6, 2004
arXiv (Cornell University), Feb 10, 2004
arXiv (Cornell University), Oct 9, 2001
arXiv (Cornell University), Oct 9, 2001
Progress of theoretical and experimental physics, Nov 1, 2015
arXiv (Cornell University), May 28, 1998
Astrophysics and space science library, 1999
Progress of Theoretical and Experimental Physics, Jun 1, 1970
Progress of Theoretical and Experimental Physics, 1979
Progress of Theoretical and Experimental Physics, Oct 1, 2001
Monthly Notices of the Royal Astronomical Society, Mar 1, 2000
Monthly Notices of the Royal Astronomical Society, Dec 1, 1987
Monthly Notices of the Royal Astronomical Society, Jun 1, 1987
Progress of Theoretical and Experimental Physics, 2015
The time-steady equation for a 1D wind accretion flow, i.e. the Bondi-Hoyle-Lyttleton (BHL) equat... more The time-steady equation for a 1D wind accretion flow, i.e. the Bondi-Hoyle-Lyttleton (BHL) equation, is investigated analytically. The BHL equation is well known to have infinitely many solutions. Traditionally, the accretion radius has been assumed to be 2GM/v 2 ∞ , but its mathematical foundation has not been clarified because of the non-uniqueness of the solution. Here, we assume that the solution curves possess physically nice characteristics, i.e. velocity and line mass-density increase monotonically with radial distance. This condition restricts the accretion radius to the range (0.71 − 1.0) × 2GM/v 2 ∞. Further assumptions, specifically, that the solution curves for velocity and line mass-density are convex upward, restrict the accretion radius to (0.84 − 0.94) × 2GM/v 2 ∞ , and 0.90 × 2GM/v 2 ∞ , respectively. Therefore, we conclude that the accretion radius is almost uniquely determined to be 0.90 × 2GM/v 2 ∞ .
On essaie de determiner dans quelle mesure la trainee sur un corps depend de la force gravitation... more On essaie de determiner dans quelle mesure la trainee sur un corps depend de la force gravitationnelle, afin d'evaluer l'echelle de temps correcte de la croissance des planetes
Symposium - International Astronomical Union
The Direct Simulation Monte Carlo (DSMC) method, developed originally to calculate rarefied gas d... more The Direct Simulation Monte Carlo (DSMC) method, developed originally to calculate rarefied gas dynamical problems, is applied to continuous flow including shocks assuming that the Knudsen number is sufficiently small. In particular, we study the formation of spiral shocks in the accretion disc of a close binary system. The method involves viscosity and thermal conduction automatically, and can thus simulate turbulent viscosity.
Monthly Notices of the Royal Astronomical Society
Monthly Notices of the Royal Astronomical Society
Monthly Notices of the Royal Astronomical Society