Hydrodynamic Characteristics and Supercavity Shape of Supercavitating Projectiles Launched with Supersonic Speed
Chuang Huang , Kaixin Guo , Kan Qin , Kai Luo , Daijin Li , Jianjun Dang
Journal of Marine Science and Application ›› 2022, Vol. 21 ›› Issue (2) : 24 -33.
A supercavitating projectile is launched underwater with supersonic speed, and then, the speed decreases to transonic and subsonic conditions orderly because of the drag coming from surrounding water. The flow regime and hydrodynamic characteristics are significantly influenced by the flying speed, the influence laws in supersonic, transonic, and subsonic regions are totally different. These issues aren’t well studied. A numerical model consisting of VOF model, moving frame method and state equation of liquid is established to calculate the compressible supercavitation flow field, and validated by comparing with a published result. The influences of water compressibility and Mach number on supercavity shape and hydrodynamic characteristics are quantitatively summarized. The results show that the flying speed of supercavitating projectiles exerts significant influences on the flow regime, supercavity shape and hydrodynamic characteristics for the transonic and supersonic conditions. With the decrease of flying speed, the drag coefficient decreases gradually, and the dimensions of the supercavity near supercavitating projectiles significantly increases in the high-speed conditions. An underwater bow shock is numerically observed before the disk cavitator in supersonic condition. However, no obvious changes are found for the incompressible water cases with different speeds. For supersonic conditions, the supercavity near supercavitating projectiles of compressible water is smaller than that of incompressible water, the drag coefficient is larger, and the relative difference significantly increases with the flying speed. For the case of Ma 1.214, the relative difference of supercavity diameter at the tail section 3.98%, and the difference of the drag coefficient is 23.90%.
Supersonic projectiles / Compressible water / Underwater shock wave / Supercavity / Hydrodynamic characteristics
| [1] |
|
| [2] |
|
| [3] |
|
| [4] |
|
| [5] |
Jenkins A, Evans T (2004) Sea mine neutralization using the an/aws-2 rapid airborne mine clearance system. 2004 IEEE Aerospace Conference Proceedings, Big Sky, MT, United States, 2999–3005 |
| [6] |
|
| [7] |
|
| [8] |
|
| [9] |
|
| [10] |
|
| [11] |
Savchenko, Y (2001) Supercavitation — problems and perspectives. Fourth International Symposium on Cavitation, Pasadena, CA USA, CAV2001: lecture.003 |
| [12] |
|
| [13] |
|
| [14] |
|
| [15] |
Serebryakov V (2001) Some Models of prediction of supercavitation Flows Based on Slender Body Approximation. Proceedings of CAV2001, CA, Pasadena, USA, CAV2001: session B3.001 |
| [16] |
Serebryakov V (2003) Some problems of hydrodynamics for sub and supersonic motion in water with supercavitation. Fifth International Symposium on Cavitation, Osaka, Japan, Cav03-OS7-015 |
| [17] |
Serebryakov V, Kirschner I, Schner G (2009a) High speed motion in water with supercavitation for sub-, trans-, supersonic Mach Numbers. Proceedings of the 7th International Symposium on Cavitation, Michigan, United States, No. 72: 1–18 |
| [18] |
Serebryakov V (2009b) Physical mathematical bases of the principle of independence of cavity expansion. Proceedings of the 7th International Symposium on Cavitation, Ann Arbor, Michigan, US, No.169: 1–14 |
| [19] |
|
| [20] |
|
| [21] |
|
| [22] |
|
| [23] |
|
/
| 〈 |
|
〉 |