gonzales computational analysis

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INDIAN HEAD Computational Analysis of a Rocket Motor Thrust Control Unit David R. González Indian Head Division, NSWC Propulsion Branch, Code E313K [email protected] 301.744.1513 Christopher Hovland Indian Head Division, NSWC Propulsion Branch, Code E313O [email protected] 301.744.6719 Distribution A: Approved for Public Release

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INDIAN HEAD

Computational Analysis of a Rocket Motor Thrust Control Unit

David R. GonzálezIndian Head Division, NSWC

Propulsion Branch, Code E313K

[email protected]

301.744.1513

Christopher HovlandIndian Head Division, NSWC

Propulsion Branch, Code E313O

[email protected]

301.744.6719

Distribution A: Approved for Public Release

Agenda

• System Overview• Analysis Objective• Analysis Approach

• Solid Model Development• Computational Fluid Dynamics Model

• Results• Thrust• Tab Surface Parameters• Flow Visualizations

• Closing Remarks

System Overview

• Nulka Active Decoy• Provides rapid response against a wide

array of anti-ship missiles.• Capable of achieving accurate placement

to provide the most effective coverage.• Emulates the radar signature of cruiser-

size ships.• Very unique flight envelope to achieve the

hovering flight.• Thrust Control Unit attached aft of the nozzle

to both position the unit and keep it stationary.

• Stringent performance characteristics must be achieved.

Analysis Objective

• Gain a better understanding of TCU behavior.• Several unexpected performance trends have been evident in static firings over the course

of the years:1. Slow Thrust Control Unit (TCU) tab response times;2. Reduced spoilage levels; &3. Thrust spoilage level reductions throughout a motor firing.

• Computational Fluid Dynamics (CFD) analyses will be conducted to investigate possible contributors.

Low Thrust Spoilage and Spoilage Reduction vs. Time.

Analysis Approach Solid Model Development

• Simplified geometry• Nominal drawing dimensions

• Several components ignored• TCU Motor;• Extender Pins; etc.

Nozzle

Deflector/Heat Shield

Tabs

Tab HingeNulka Propulsion Unit Nulka Derived Solid Model

Analysis Approach Computational Fluid Dynamics Model

• Domain of interest must be broken into small, discrete elements (computational mesh).

• Domain includes:1. Solid model geometry (solid surfaces); &2. Fluid domain.

• Individual models must be built for each insertion configuration of interest.

• Two software have been used both for model verification and for the analysis of different TCU dynamics:

1. Full, 360° circumferential model (includes all 3 thrust tabs) using Fluent; &

2. 120° circumferential symmetry model (only 1 thrust tab) using AVUS.• These are discussed in the following slides.

Analysis Approach Computational Fluid Dynamics Model

• Fluent• Initial version (used for model verification)

1. Truncated thrust tabs;2. No chassis towers included.

• TCU Performance Study version1. Full, solid model geometry

CFD Model used for Verification

Full-geometry CFD Model

Analysis Approach Computational Fluid Dynamics Model

• AVUS• 120°-Symmetry model.• Includes a single thrust tab (full solid

model geometry).• Can only be used to account for

symmetric insertions

Symmetry Lines

120° Symmetry Model

Rocket motor case not pictured.

Analysis Approach Computational Fluid Dynamics Model

• Conventions• Positive Tab Moment = Tab Tendency to Extract (insert further into efflux; left

figure).• Tab Surface Pressures and Temperatures measured along face centerline from

bottom up (right figure).

Positive Tab Arm Moment

Analysis Approach Computational Fluid Dynamics Model

• Predicted Results1. Axial thrust / Thrust spoilage;2. Forces & Moments

• Tab Face / Tab Arm Contributions;• Pressure and Viscous Components;• Etc.

3. Surface Pressures & CP• Along tab face.• CP used as measure of Mach disk

location.

4. Surface Temperatures• Along tab face.• Temperature contours shown for

remainder of tab geometry.

Readily measured in static firings.

Very difficult (near impossible) to instrument a motor to collect these measurements.

Thrust-Time HistoryTest Firing Data

Time

Thru

st

Firing AFiring B

Results LAT Data Points Simulated

• Two sets of PU LAT firing data provided for model verification.• Firing A (cold-conditioned motor; low pressure);• Firing B (hot-conditioned motor; high pressure).

1

2

3

4

• Data points chosen for strategic value in demonstrating different aspects of TCU performance:– Firing A (low pressure)

1. Ballistic performance (thrust retracted);

2. Full tab insertion;3. Asymmetric tab insertion

– Firing B (high pressure)4. Full tab insertion.

• CFD conducted using Fluent, except 1.

Results Thrust

• Thrust Predictions– Key Findings:

• Ballistic thrust levels were predicted with great accuracy; • CFD predicted higher levels of thrust spoilage than observed in LAT;• CFD aptly captures the flow physics (verified by good agreement with thrust levels).

Thrust-Time HistoryFiring A Test Data

Time

Thru

st

Firing A Corrected ThrustFirinig AMax Spoilage LimitCFD

Thrust-Time HistoryFiring B Test Data

Time

Thru

st

Firing B Corrected ThrustFiring BCFD

Results Surface Pressures

• Tab Surface Pressures (Click for tab surface pressure visualizations)

– Key Findings:1. Mach disk imposes almost a constant pressure level on inserted portion of tab face;2. Max pressure for all insertions corresponded to oblique shock impingement point;3. Pressures levels before and after oblique shock impingement in the asymmetric insertion are

reduced because of the lack of shock convergence.R1 Surface Pressures

Distance

Pres

sure

Full, Lo PFull, Hi PAsym, Lo P

Results Center-of-Pressure

• Centers-of-Pressure (Click for tabular results)

– Key Findings:1. Full symmetric insertions (low and high pressure) had almost identical CP placements (owing to the

near identical surface pressure profile);2. CP located below hinge line at the full symmetric insertions, generating the positive moments;3. Since oblique shock impingement is the biggest source of pressure on the asymmetric insertion, CP for

this case is located further up the tab, creating a negative moment.

NOTE:Color contours DO NOT reflect any data relevant to the CP data being presented. They are meant as a means to distinguish the tab face from the rest of the geometry.

Full, Lo P Full, Hi P Asym, Lo P

Tab Surface Temperatures

0

500

1000

1500

2000

2500

3000

3500

0 2 4 6 8 10 12 14 16

Distance (mm)

Tem

pera

ture

(K)

13.6 mm - Lo P13.6 mm - Hi P12.5 mm - R112.5 mm - R2

Results Surface Temperatures

• Tab Surface Temperatures (Click for visualizations of temperature around thrust tabs)

– Key Findings:1. Full chamber temperature recovered on all inserted tabs;2. Temperatures peaked in regions not exposed to high pressures in symmetric insertions. These were

found to be due to the accelerating flow between the tab and nozzle , generating reduced gas densities (Click to view profile).

3. Asymmetric tab experiences slightly higher temperatures at the bottom of the tab face;

4. Elevated temperatures found on retracted tabs due to thrust vectoring.

Results Mach Iso-Surfaces

• Exhaust Plume Visualizations

Mach Contours Along Centerline (Retracted Tabs).

Mach 1 & 2 Iso-Surfaces for Full Insertion @ Low Pressure.

Mach 1 & 2 Iso-Surfaces for Full Insertion @ High Pressure.

Mach 1 & 2 Iso-Surfaces for Asymmetric Insertion @ Low Pressure.

Results Mach Disk Location

• Predicted Mach Disk

Concluding Remarks

• Computational fluid dynamic (CFD) models have been shown to correctly predict the complicated flow physics of the Thrust Control Unit.

• Two versions were developed that made use of simplified geometry. 1. Full circumferential model

(incorporating all 3 tabs); &2. 120° symmetry model (single tab

incorporated).

• CFD models allow for the study of parameters not easily obtained in experimental setups, including:

1. Tab forces and moments;2. Tab surface pressures;3. Tab surface temperatures;4. Mach disk location;5. Etc.

• Thrust/Spoilage can also be predicted.

Concluding Remarks

• Axial thrust and thrust spoilage magnitudes were found to agree well with FSED- specified levels.

• Moment magnitudes were found to be comparable to those predicted by the current performance model.

• Tab arms were found to have significant contributions to total moment magnitudes;• Current performance model neglects the tab arm contribution.

• Tab face surface temperatures were found to be around the magnitude of the combustion chamber.

• Majority of tab arm was predicted to be at or around atmospheric temperature;• At full insertion, accelerated flow between tab face and nozzle was at higher

temperature than at the surface exposed to efflux due to the reduced density;• Lower insertions did not exhibit a similar behavior.

Concluding Remarks

• FY09 work will focus on continuing the systematic analysis of the TCU. This will include:

1. Further TCU performance characterization at high pressure extreme;2. Asymmetric insertions; &3. Spoilage sensitivities.

• Performance trends and TCU responses identified from these series of investigations can later be incorporated into available performance models.

Backup Slides

Results - Backup Model Verification Runs

• Thrust Tab Face Surface Pressures (Back to main presentation)

Full Insertion @ Low Pressure. Full Insertion @ High Pressure.

Asymm. Insertion @ Low Pressure.

Results - Backup Model Verification Runs

• Thrust Tab Surface Temperature Contours (Back to main presentation)

Symmetric Insertion Temperature Contours: (l) Lo P; (r) Hi P.

Asymmetric Insertion Temperature Contours: (l) R1; (r) R3.

Results - Backup Model Verification Runs

• Temperatures Between Nozzle & Tab for Max. Symmetric Insertion (Back to main presentation)

For a Perfect Gas:

RpTρ

=

p = atmospheric pressure;

R = the gas constant.

Gas Density on Tab Surface

Distance

Den

sity

Full - Lo P

Flow Entrainment Visuals