Rocket thrust equation in under-expanded nozzle

In summary: With an over-expanded nozzle, the pressure inside the nozzle falls below ambient pressure. This causes a decrease in thrust. However, as long as the over-expanded condition does not persist (i.e. the pressure inside the nozzle equals atmospheric pressure), the engine will operate at its optimal condition and produce the highest possible thrust and specific impulse.
  • #1
pejsek
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TL;DR Summary
How does the rocket thrust equation work for under-expanded nozzle where the pressure component of thrust becomes positive and thrust should then be higher?
Hello,

so the thrust equation goes like: F = (m dot)*v_e + A_e*(p_e - p_a), where

F ... thrust [N]
m dot ... mass flow rate [kg/s]
v_e ... velocity of exhaust [m/s]
A_e ... area of the exit nozzle plane [m2]
p_e ... pressure of the exhaust at the exit of the nozzle [Pa(a)]
p_a ... ambient pressure [Pa(a)]

We know that if p_e < p_a the pressure component in the equation will be negative and thrust will go down. That is the case of over-expanded nozzle. If p_e = p_a the pressure component is zero and as every rocket physics book says, the flow through the nozzle has reached its optimal condition. This is where thrust and specific impulse reach their maximum.

It is well known that the maximum thrust and specific impulse of a nozzle is in vacuum, as is evident from the picture below taken from the book Fundamentals of Rocket Propulsion by D.P. Mishra.

1683115346225.png


My question is, how does this fact translate into the thrust equation? For p_e > p_a the pressure component would become positive and add some thrust. But clearly that's not what happens. I was thinking maybe v_e gets smaller, but v_e seems to be function of p_e but not p_a, according to this equation:

1683133354820.png


p_e is affected by p_a though, but only when the nozzle is highly over-expanded and a shock wave occurs inside the nozzle. If p_e > p_a then the exhaust can expand no more inside the nozzle (the nozzle is "too short") and so p_e no longer decreases. In the same book, the author gives this example calculation:

1683135432633.png

1683134088222.png


where he adds the pressure component to the total thrust. If we substituted the value p_a = 5.53 kPa with the value p_a = p_e = 105 kPa (I know it's weird) which would be the ideal nozzle condition, then the pressure component of thrust would be zero and apparently the total thrust would be lower. So where is the catch?

Thank you for any replies,
pejsek
 
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  • #2
The equation you have cited for exhaust velocity is not impacted by atmospheric conditions at all. You make the statement that the exhaust pressure is impacted by atmospheric pressure, and that is incorrect. Regardless of whether you are operating the engine at sea level, or in a vacuum, that exhaust velocity is set in stone.

The corrections and losses to thrust that you are seeking in that equation, actually do not reside in that equation. The answer to your question resides in the even-simpler thrust equation:

Capture.JPG


You mentioned shock waves occurring in the nozzle impacting all of these models- you are correct. However, the moment shocks are forming in your nozzle and you have flow detachment, you can throw away every single one of the equations you see in this thread. Now you're talking about a state that the engine was not designed for, and it has failed. Time to shrug your shoulders, give up on modeling it, and figure out what went wrong with your engine.
 
  • #3
You still gain a little bit of thrust as the outside pressure keeps decreasing as your formulas show, but a larger nozzle would increase the exhaust velocity and provide more thrust: The engine becomes inefficient in the sense that it doesn't use the full potential of the propellant.
 

What is the rocket thrust equation?

The rocket thrust equation, also known as the Tsiolkovsky rocket equation, is a mathematical formula that describes the relationship between the mass of a rocket, its velocity, and the amount of fuel it carries. It is given by the equation: T = Ve * ln(M0/Mf), where T is the thrust, Ve is the effective exhaust velocity, M0 is the initial mass of the rocket, and Mf is the final mass of the rocket.

What is an under-expanded nozzle?

An under-expanded nozzle is a type of rocket nozzle where the exit pressure is lower than the ambient pressure. This results in the exhaust gases expanding rapidly upon exiting the nozzle, creating a shock wave. This type of nozzle is commonly used in rocket engines for high altitude flights.

How does the rocket thrust equation apply to under-expanded nozzles?

The rocket thrust equation can be used to calculate the thrust produced by an under-expanded nozzle. The effective exhaust velocity, Ve, is affected by the ambient pressure and the exit pressure of the nozzle. As the exit pressure decreases, the effective exhaust velocity increases, resulting in a higher thrust.

What factors affect the thrust produced by an under-expanded nozzle?

The thrust produced by an under-expanded nozzle is affected by several factors, including the ambient pressure, the exit pressure, the nozzle geometry, and the propellant flow rate. As mentioned before, a lower exit pressure and a higher ambient pressure will result in a higher thrust. The nozzle geometry also plays a role in determining the amount of thrust, as a well-designed nozzle can increase the efficiency of the exhaust gases. Lastly, the propellant flow rate affects the thrust by determining the amount of mass that is expelled from the nozzle per unit time.

How is the rocket thrust equation used in rocket design?

The rocket thrust equation is an essential tool in rocket design, as it allows engineers to calculate the thrust produced by different types of nozzles and propellants. By using this equation, they can optimize the design of the nozzle and the propellant flow rate to achieve the desired thrust for a specific rocket. It is also useful in determining the maximum achievable velocity and altitude for a rocket based on its mass and fuel capacity.

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