Combustion Instability in F-1 Engine - gatech.edu

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1 LRE Combustion Instability -1 Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion LRE Combustion Instability Some Basics LRE Combustion Instability -2 Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion Combustion Instability in F-1 Engine Typical combustion instabilities observed in early F-1 engines resurges 5000 psi Chamber Pressure from V. Yang time

Transcript of Combustion Instability in F-1 Engine - gatech.edu

Page 1: Combustion Instability in F-1 Engine - gatech.edu

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LRE Combustion Instability -1

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

LRE Combustion Instability

Some Basics

LRE Combustion Instability -2

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Combustion Instability in F-1 Engine

• Typical combustion instabilities observed in

early F-1 engines

resurges

5000 psi

Chamber Pressure

from V. Yangtime

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LRE Combustion Instability -3

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Acoustic Pressure Oscillations

• Can approach them from point-of-view of

dynamic system modeling

after Culick and Yang, Overview of Combustion Instabilities in Liquid Propellant Rocket Engines

Limit Cycle

tFpdt

pd

dt

pdo

2

2

2

2

F(t)

Forcing Function

ResonantFrequency

Gain/Damping

LRE Combustion Instability -4

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Feedback Loops in Combustion Instability

from T. Lieuwen

q

p

t

0'' dtqp

Rayleigh’s Criterion

• Gas that burns (heat

release) expands,

and generates

compression waves

for amplification of oscillations

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LRE Combustion Instability -5

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Combustion Driving

• Ways that heat release can be made to

fluctuate and lock-in to pressure oscillations

– bulk reactant flowrates respond to pinjection

• can also impact atomization

• interact with pump cavitation

– acoustic pressure fluctuations correlate to

acoustic velocity fluctuations

• can impact flow within injectors and

downstream of injectors

• alters atomization, mixing, flame stabilization

LRE Combustion Instability -6

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Acoustic Resonances

• C.C. Longitudinal modes

– f a/L

• C.C. Transverse modes

– radial and azimuthal/tangential

– f a/R

• Injector and manifold resonances

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LRE Combustion Instability -7

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Frequency Based Nomenclature

• Chugging

– low freq: f ~10-400 Hz

– often related to propellant feed system oscillations

• Screeching (screaming)

– high freq: f > 1 kHz

– typically contains highest energy, most damaging

• Buzzing

– intermediate frequencies

LRE Combustion Instability -8

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

LRE Combustion Instability

Suppression

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LRE Combustion Instability -9

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Main Combustion Chamber Dynamics

acoustic driver

flow distributor

GOX

pressure transducerspressure transducers

p-

p+

pt-

𝛻2𝑝′ −1

𝑎2

𝜕2𝑝′

𝜕𝑡2= ℎ ≡ linear + nonlinear sources

𝐧 ∙ 𝛻𝑝′ = −𝑓 along boundaries

RD-170 Main Chamber Assembly from V. Yang

LRE Combustion Instability -10

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Combustion Instability PreventionRD-170 Main Chamber Assembly

Line 1 – Stable Combustion

Line 2 – Injector/Baffle Damping

Line 3 – Distributor Damping

Line 4 – Acoustic

Cavities

from V. Yang

• Baffles suppress

transverse

modes

• Perforated

plate

reduces

feedback

to supply

system

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LRE Combustion Instability -11

Copyright © 2019 by Jerry M. Seitzman. All rights reserved. AE6450 Rocket Propulsion

Acoustic Cavities - Helmholtz Resonators

• Cavity acts to absorb pressure

fluctuations from high p part of cycle

and return it during low p

– also produces jet leaving orifice

that provides viscous damping

• Often placed

– near injectors

• important to suppress oscillations

there

– in corners

• near pressure anti-node (spatial

location with large p)

AVL

af

2

1

AV

L