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    АСродинамичкС карактСристикС осносимСтричних Ρ‚Π΅Π»Π° Ρƒ нСсимСтричном ΡΡ‚Ρ€ΡƒΡ˜Π½ΠΎΠΌ ΠΏΠΎΡ™Ρƒ

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    ΠŸΡ€ΠΈΠΊΠ°Π·Π°Π½Π΅ су основнС Ρ˜Π΅Π΄Π½Π°Ρ‡ΠΈΠ½Π΅ Ρ‚ΡƒΡ€Π±ΡƒΠ»Π΅Π½Ρ‚Π½ΠΎΠ³ ΡΡ‚Ρ€ΡƒΡ˜Π°ΡšΠ°. ΠŸΡ€Π΅Π·Π΅Π½Ρ‚ΠΎΠ²Π°Π½Π° јС ΠΈ ΠΏΡ€ΠΈΠΌΠ΅ΡšΠ΅Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π‘ΠΏΠ°Π»Π°Ρ€Ρ‚Π° ΠΈ Алмараса. ΠŸΡ€ΠΎΡ€Π°Ρ‡ΡƒΠ½ јС Π²Ρ€ΡˆΠ΅Π½ Π½Π° Π°Π΄Π°ΠΏΡ‚ΠΈΠ²Π½ΠΎΡ˜ ΠΏΡ€ΠΎΡ€Π°Ρ‡ΡƒΠ½ΡΠΊΠΎΡ˜ ΠΌΡ€Π΅ΠΆΠΈ. ΠˆΠ΅Π΄Π½Π°Ρ‡ΠΈΠ½Π° ΠΏΠΎ притиску јС ΠΊΠΎΡ€ΠΈΡˆΡ›Π΅Π½Π° Π·Π° ΠΎΡΡ‚Π²Π°Ρ€ΠΈΠ²Π°ΡšΠ΅ ΠΊΠΎΠ½Π²Π΅Ρ€Π³Π΅Π½Ρ†ΠΈΡ˜Π΅ Ρ€Π΅ΡˆΠ΅ΡšΠ°. Π˜Π·Π²Ρ€ΡˆΠ΅Π½ΠΈ су ΠΏΡ€ΠΎΡ€Π°Ρ‡ΡƒΠ½ΠΈ Π·Π° Ρ€Π°Π·Π»ΠΈΡ‡ΠΈΡ‚Π΅ Π½Π°ΠΏΠ°Π΄Π½Π΅ ΡƒΠ³Π»ΠΎΠ²Π΅ ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡ΠΈΡ‚Π΅ ΠΎΡ‚ΠΊΠ»ΠΎΠ½Π΅ ΠΊΠΎΠΌΠ°Π½Π΄Π½ΠΈΡ… ΠΏΠΎΠ²Ρ€ΡˆΠΈΠ½Π°. Π Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈ добијСни ΠΏΡ€ΠΎΡ€Π°Ρ‡ΡƒΠ½ΠΎΠΌ су ΡƒΠΏΠΎΡ€Π΅Ρ’Π΅Π½ΠΈ са Ρ€Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈΠΌΠ° добијСним аСротунСлским ΠΌΠ΅Ρ€Π΅ΡšΠΈΠΌΠ°. Описано јС СкспСримСнтално ΠΏΠΎΡΡ‚Ρ€ΠΎΡ˜Π΅ΡšΠ΅ ΠΈ ΠΌΠΎΠ΄Π΅Π» ΠΈΡΠΏΠΈΡ‚ΠΈΠ²Π°ΡšΠ°. Π Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈ су ΠΏΡ€ΠΈΠΊΠ°Π·Π°Π½ΠΈ Π΄ΠΈΡ˜Π°Π³Ρ€Π°ΠΌΠΈΠΌΠ° Π°Π΅Ρ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡ‡ΠΊΠΈΡ… ΠΊΠΎΠ΅Ρ„ΠΈΡ†ΠΈΡ˜Π΅Π½Π°Ρ‚Π° ΠΈ Π΄ΠΈΡ˜Π°Π³Ρ€Π°ΠΌΠΈΠΌΠ° расподСлС Π±Ρ€Π·ΠΈΠ½Π΅, притиска ΠΈ ΠΌΠ°Ρ…ΠΎΠ²ΠΈΡ… Π±Ρ€ΠΎΡ˜Π΅Π²Π°.Governing equations for turbulent flows are reviewed. Spalart Allmaras turbulence model has been selected for aerodynamic calculations. Computation is performed on the adaptive computational grid. Pressure based method for computational convergence was selected. Computations were performed for various angles of attack and various command surface deflections. Calculated results were compared with results obtained by wind tunnel testing. Experimental setup and experimental model are described. Results are presented by aerodynamic coefficients and contour lines of the Mach numbers, pressures and velocities

    Aerodynamic characteristic of a canard guided rocket

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