From Wikipedia, the free encyclopedia - View original article

(Redirected from Laval nozzle)

A **de Laval nozzle** (or **convergent-divergent nozzle**, **CD nozzle** or **con-di nozzle**) is a tube that is pinched in the middle, making a carefully balanced, asymmetric hourglass-shape. It is used to accelerate a hot, pressurized gas passing through it to a supersonic speed, and upon expansion, to shape the exhaust flow so that the heat energy propelling the flow is maximally converted into directed kinetic energy. Because of this, the nozzle is widely used in some types of steam turbines, and is used as a rocket engine nozzle. It also sees use in supersonic jet engines.

Similar flow properties have been applied to jet streams within astrophysics.^{[1]}

The nozzle was developed by Swedish inventor Gustaf de Laval in 1888 for use on a steam turbine.^{[2]}^{[3]}^{[4]}^{[5]}

This principle was first used in a rocket engine by Robert Goddard. Very nearly all modern rocket engines that employ hot gas combustion use de Laval nozzles.

Its operation relies on the different properties of gases flowing at subsonic and supersonic speeds. The speed of a subsonic flow of gas will increase if the pipe carrying it narrows because the mass flow rate is constant. The gas flow through a de Laval nozzle is isentropic (gas entropy is nearly constant). At subsonic flow the gas is compressible; sound, a small pressure wave, will propagate through it. At the "throat", where the cross sectional area is a minimum, the gas velocity locally becomes sonic (Mach number = 1.0), a condition called choked flow. As the nozzle cross sectional area increases the gas begins to expand and the gas flow increases to supersonic velocities where a sound wave will not propagate backwards through the gas as viewed in the frame of reference of the nozzle (Mach number > 1.0).

A de Laval nozzle will only choke at the throat if the pressure and mass flow through the nozzle is sufficient to reach sonic speeds, otherwise no supersonic flow is achieved and it will act as a Venturi tube; this requires the entry pressure to the nozzle to be significantly above ambient at all times (equivalently, the stagnation pressure of the jet must be above ambient).

In addition, the pressure of the gas at the exit of the expansion portion of the exhaust of a nozzle must not be too low. Because pressure cannot travel upstream through the supersonic flow, the exit pressure can be significantly below ambient pressure it exhausts into, but if it is too far below ambient, then the flow will cease to be supersonic, or the flow will separate within the expansion portion of the nozzle, forming an unstable jet that may 'flop' around within the nozzle, possibly damaging it.

In practice ambient pressure must be no higher than roughly 2-3 times the pressure in the supersonic gas at the exit for supersonic flow to leave the nozzle.

The analysis of gas flow through de Laval nozzles involves a number of concepts and assumptions:

- For simplicity, the gas is assumed to be an ideal gas.
- The gas flow is isentropic (i.e., at constant entropy). As a result the flow is reversible (frictionless and no dissipative losses), and adiabatic (i.e., there is no heat gained or lost).
- The gas flow is constant (i.e., steady) during the period of the propellant burn.
- The gas flow is along a straight line from gas inlet to exhaust gas exit (i.e., along the nozzle's axis of symmetry)
- The gas flow behavior is compressible since the flow is at very high velocities (Mach number > 0.3).

As the gas enters a nozzle, it is moving at subsonic velocities. As the throat contracts, the gas is forced to accelerate until at the nozzle throat, where the cross-sectional area is the smallest, the axial velocity becomes sonic. From the throat the cross-sectional area then increases, the gas expands and the axial velocity becomes progressively more supersonic.

The linear velocity of the exiting exhaust gases can be calculated using the following equation:^{[6]}^{[7]}^{[8]}

where: | |

= Exhaust velocity at nozzle exit, m/s | |

= absolute temperature of inlet gas, K | |

= Universal gas law constant = 8314.5 J/(kmol·K) | |

= the gas molecular mass, kg/kmol (also known as the molecular weight) | |

= = isentropic expansion factor | |

= specific heat of the gas at constant pressure | |

= specific heat of the gas at constant volume | |

= absolute pressure of exhaust gas at nozzle exit, Pa | |

= absolute pressure of inlet gas, Pa |

Some typical values of the exhaust gas velocity *v*_{e} for rocket engines burning various propellants are:

- 1,700 to 2,900 m/s (3,800 to 6,500 mph) for liquid monopropellants
- 2,900 to 4,500 m/s (6,500 to 10,100 mph) for liquid bipropellants
- 2,100 to 3,200 m/s (4,700 to 7,200 mph) for solid propellants

As a note of interest, * v_{e}* is sometimes referred to as the

As an example calculation using the above equation, assume that the propellant combustion gases are: at an absolute pressure entering the nozzle of * p* = 7.0 MPa and exit the rocket exhaust at an absolute pressure of

The technical literature can be very confusing because many authors fail to explain whether they are using the universal gas law constant * R* which applies to any ideal gas or whether they are using the gas law constant

- Choked flow
- Giovanni Battista Venturi
- Gustaf de Laval
- History of the internal combustion engine
- Nozzle
- Rocket engine
- Rocket engine nozzles
- Spacecraft propulsion
- Twister Supersonic Separator for natural gas treatment
- Venturi tube
- Venturi effect
- Isentropic nozzle flow

Wikimedia Commons has media related to .Convergent-divergent nozzles |

**^**C.J. Clarke and B. Carswell (2007).*Principles of Astrophysical Fluid Dynamics*(1st ed.). Cambridge University Press. p. 226. ISBN 978-0-521-85331-6.**^**British patent 7143 of 1889.**^**Theodore Stevens and Henry M. Hobart (1906).*Steam Turbine Engineering*. MacMillan Company. pp. 24–27. Available on-line here in Google Books.**^**Robert M. Neilson (1903).*The Steam Turbine*. Longmans, Green, and Company. pp. 102–103. Available on-line here in Google Books.**^**Garrett Scaife (2000).*From Galaxies to Turbines: Science, Technology, and the Parsons Family*. Taylor & Francis Group. p. 197. Available on-line here in Google Books.**^**Richard Nakka's Equation 12.**^**Robert Braeuning's Equation 1.22.**^**George P. Sutton (1992).*Rocket Propulsion Elements: An Introduction to the Engineering of Rockets*(6th ed.). Wiley-Interscience. p. 636. ISBN 0-471-52938-9.