Physics

Jet propulsion is produced by some reaction engines or animals when thrust is generated by a fast moving jet of fluid in accordance with Newton's laws of motion. It is most effective when the Reynolds number is high—that is, the object being propelled is relatively large and passing through a low-viscosity medium.[1]

In animals, the most efficient jets are pulsed, rather than continuous,[2] at least when the Reynolds number is greater than 6.[3]

Specific impulse

Specific impulse (usually abbreviated Isp) is a measure of how effectively a rocket uses propellant or jet engine uses fuel. By definition, it is the total impulse (or change in momentum) delivered per unit of propellant consumed[4] and is dimensionally equivalent to the generated thrust divided by the propellant mass flow rate or weight flow rate.[5] If mass (kilogram, pound-mass, or slug) is used as the unit of propellant, then specific impulse has units of velocity. If weight (newton or pound-force) is used instead, then specific impulse has units of time (seconds). Multiplying flow rate by the standard gravity (g0) converts specific impulse from the mass basis to the weight basis.[5]

A propulsion system with a higher specific impulse uses the mass of the propellant more effectively in creating forward thrust and, in the case of a rocket, less propellant needed for a given delta-v, per the Tsiolkovsky rocket equation.[4][6] In rockets, this means the engine is more effective at gaining altitude, distance, and velocity. This effectiveness is less important in jet engines that employ wings and use outside air for combustion and carry payloads that are much heavier than the propellant.

Specific impulse includes the contribution to impulse provided by external air that has been used for combustion and is exhausted with the spent propellant. Jet engines use outside air, and therefore have a much higher specific impulse than rocket engines. The specific impulse in terms of propellant mass spent has units of distance per time, which is an artificial velocity called the "effective exhaust velocity". This is higher than the actual exhaust velocity because the mass of the combustion air is not being accounted for. Actual and effective exhaust velocity are the same in rocket engines not utilizing air.

Specific impulse is inversely proportional to specific fuel consumption (SFC) by the relationship Isp = 1/(go·SFC) for SFC in kg/(N·s) and Isp = 3600/SFC for SFC in lb/(lbf·hr).

Thrust

From the definition of specific impulse thrust in SI units is:

${\displaystyle F={\dot {m}}V_{e}}$

where Ve is the effective exhaust velocity and ${\displaystyle {\dot {m}}}$ is the propellant flow rate.

Jet-propelled animals

Cephalopods such as squid use jet propulsion for rapid escape from predators; they use other mechanisms for slow swimming. The jet is produced by ejecting water through a siphon, which typically narrows to a small opening to produce the maximum exhalent velocity. The water passes through the gills prior to exhalation, fulfilling the dual purpose of respiration and locomotion.[1] Sea hares (gastropod molluscs) employ a similar method, but without the sophisticated neurological machinery of cephalopods they navigate somewhat more clumsily.[1]

Some teleost fish have also developed jet propulsion, passing water through the gills to supplement fin-driven motion.[7]: 201

In some dragonfly larvae, jet propulsion is achieved by the expulsion of water from a specialised cavity through the anus. Given the small size of the organism, a great speed is achieved.[8]

Scallops and cardiids,[9] siphonophores,[10] tunicates (such as salps),[11][12] and some jellyfish[13][14][15] also employ jet propulsion. The most efficient jet-propelled organisms are the salps,[11] which use an order of magnitude less energy (per kilogram per metre) than squid.[16]

Discover more about Jet-propelled animals related topics

Source: "Jet propulsion", Wikipedia, Wikimedia Foundation, (2023, February 26th), https://en.wikipedia.org/wiki/Jet_propulsion.

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References
1. ^ a b c Packard, A. (1972). "Cephalopods and Fish: the Limits of Convergence". Biological Reviews. 47 (2): 241–307. doi:10.1111/j.1469-185X.1972.tb00975.x. S2CID 85088231.
2. ^ Sutherland, K. R.; Madin, L. P. (2010). "Comparative jet wake structure and swimming performance of salps" (PDF). Journal of Experimental Biology. 213 (Pt 17): 2967–75. doi:10.1242/jeb.041962. PMID 20709925.
3. ^ Dabiri, J. O.; Gharib, M. (2005). "The role of optimal vortex formation in biological fluid transport". Proceedings of the Royal Society B: Biological Sciences. 272 (1572): 1557–1560. doi:10.1098/rspb.2005.3109. PMC 1559837. PMID 16048770.
4. ^ a b "What is specific impulse?". Qualitative Reasoning Group. Retrieved 22 December 2009.
5. ^ a b Benson, Tom (11 July 2008). "Specific impulse". NASA. Archived from the original on 24 January 2010. Retrieved 22 December 2009.
6. ^ Hutchinson, Lee (14 April 2013). "New F-1B rocket engine upgrades Apollo-era design with 1.8M lbs of thrust". Ars Technica. Retrieved 15 April 2013. The measure of a rocket's fuel effectiveness is called its specific impulse (abbreviated as 'ISP'—or more properly Isp).... 'Mass specific impulse...describes the thrust-producing effectiveness of a chemical reaction and it is most easily thought of as the amount of thrust force produced by each pound (mass) of fuel and oxidizer propellant burned in a unit of time. It is kind of like a measure of miles per gallon (mpg) for rockets.'
7. ^ Wake, M.H. (1993). "The Skull as a Locomotor Organ". In Hanken, James (ed.). The Skull. University of Chicago Press. p. 460. ISBN 978-0-226-31573-7.
8. ^ Mill, P. J.; Pickard, R. S. (1975). "Jet-propulsion in anisopteran dragonfly larvae". Journal of Comparative Physiology. 97 (4): 329–338. doi:10.1007/BF00631969. S2CID 45066664.
9. ^ Chamberlain Jr, John A. (1987). "32. Locomotion of Nautilus". In Saunders, W. B.; Landman, N. H. (eds.). Nautilus: The Biology and Paleobiology of a Living Fossil. ISBN 9789048132980.
10. ^ Bone, Q.; Trueman, E. R. (2009). "Jet propulsion of the calycophoran siphonophores Chelophyes and Abylopsis". Journal of the Marine Biological Association of the United Kingdom. 62 (2): 263–276. doi:10.1017/S0025315400057271. S2CID 84754313.
11. ^ a b Bone, Q.; Trueman, E. R. (2009). "Jet propulsion in salps (Tunicata: Thaliacea)". Journal of Zoology. 201 (4): 481–506. doi:10.1111/j.1469-7998.1983.tb05071.x.
12. ^ Bone, Q.; Trueman, E. (1984). "Jet propulsion in Doliolum (Tunicata: Thaliacea)". Journal of Experimental Marine Biology and Ecology. 76 (2): 105–118. doi:10.1016/0022-0981(84)90059-5.
13. ^ Demont, M. Edwin; Gosline, John M. (January 1, 1988). "Mechanics of Jet Propulsion in the Hydromedusan Jellyfish, Polyorchis Pexicillatus: I. Mechanical Properties of the Locomotor Structure". J. Exp. Biol. 134 (134): 313–332. doi:10.1242/jeb.134.1.313.
14. ^ Demont, M. Edwin; Gosline, John M. (January 1, 1988). "Mechanics of Jet Propulsion in the Hydromedusan Jellyfish, Polyorchis Pexicillatus: II. Energetics of the Jet Cycle". J. Exp. Biol. 134 (134): 333–345. doi:10.1242/jeb.134.1.333.
15. ^ Demont, M. Edwin; Gosline, John M. (January 1, 1988). "Mechanics of Jet Propulsion in the Hydromedusan Jellyfish, Polyorchis Pexicillatus: III. A Natural Resonating Bell; The Presence and Importance of a Resonant Phenomenon in the Locomotor Structure". J. Exp. Biol. 134 (134): 347–361. doi:10.1242/jeb.134.1.347.
16. ^ Madin, L. P. (1990). "Aspects of jet propulsion in salps". Canadian Journal of Zoology. 68 (4): 765–777. doi:10.1139/z90-111.
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