introduction to high power rocketry
DESCRIPTION
Introduction to high power rocketry. Dr. Adam M Baker. Summary. How does HPR differ from model rocketry? Some design guidelines for HPR Something on payloads Examples of HPR Still images... Videos...HARDWARE! Amateur rocketry www.ukra.org.uk. HPR v. Model rockets (1). - PowerPoint PPT PresentationTRANSCRIPT
Introduction to high power rocketry
Dr. Adam M Baker
Summary
1. How does HPR differ from model rocketry?2. Some design guidelines for HPR3. Something on payloads4. Examples of HPR
• Still images... Videos...HARDWARE!5. Amateur rocketry
www.ukra.org.uk
HPR v. Model rockets (1)
HPR v. Model rockets (2)• ESTES • Aerotech K550W
Total Impulse 1595 (Ns) Maximum Thrust 845 (N) Average Thrust 467 (N) Burn Time 3.42 (s) Loaded Mass 1.51 (kg) Propellant Mass 0.88 (kg)
Total Impulse 5 (Ns) Maximum Thrust 12 (N) Average Thrust 6 (N) Burn Time 0.85 (s) Loaded Mass 0.018 (kg) Propellant Mass 0.065 (kg)
HPR v. Model rockets (3)
HPR v. Model rockets (4)
• Models– Paper– Balsa– Plastic
• HPR– Metals e.g. Aluminium– CFRP– Phenolic tubing
HPR v. Model rockets (5)
• Mass, Size• Motors• Trajectory• Materials, components
SAFETY
Where can I get help?
• UK Rocketry Association• www.ukra.org.uk• Rules, regs , lots of
‘experts’• ESSENTIAL for launch
• Rockets ‘n’ Things– Malcolm Jennings
• Main supplier in Southern England for HPR parts
• www.rocketsandthings.com
Guidelines
For HPR design
Stability (1)
– Defined by Barrowman equations
– Cp v. Cg, or – ‘Static margin’
http://my.execpc.com/~culp/rockets/Barrowman.htmlhttp://www.apogeerockets.com/downloads/pdfs/barrowman_report.pdf
Stability (2)
• Barrowman– Slender body theory
1. (L/D) between 10 and 35
2. 15 < CN <303. Subsonic flight. 4. ‘Thin’ cross-section fins.
• Velocity– Min 20m/s for fins to act– Or 50m/s2 acceleration
(4m launch tower / rail)Þ6:1 T:W on launch
• Static stability margin- 1.5-2.5 calibres
CENTREOF
MASS
CENTREOF
PRESSURE
1.5D<STATIC MARGIN<2.5D
L
D
Launch ramp / tower / rail
Motor mountingTotal Impulse 1595 (Ns) Maximum Thrust 845 (N) Average Thrust 467 (N) Burn Time 3.42 (s) Loaded Mass 1.51 (kg) Propellant Mass 0.88 (kg)
NUT
FIREWALL
MOTOR CASE
FORWARD BULKHEAD
CLAMP1.2.
FIN
MOTOR THRUST RING
Structure2° MAX LONGITUDINALAXIS
TEST FORCE=2 x FIN MASS x MAX ACCELERATION
d
LAUNCH WEIGHT OF ROCKET
S
d < S x tan 10°
z
x
Z/X< 1%
CENTREOF MASS
Fin alignment
Fin Long. loading
Fin Lat. loading
Structure (2)
• Coupling sections of rocket
METAL
PLASTICSor
COMPOSITE
CONNECTING BODY TUBES
1/2 D
D
D
Recovery
Recovery (2)
• Redundancy
• Test Test Test!
• Tracking
HPR Payloads
Payloads (1)
• Accelerometer / altimeter– E.g.
• G-Wiz• P-Nut
• Flight computer– E.g. R-DAS
http://www.aedelectronics.nl/rdas/
Credit: Richard Osborne
Payloads (2)
• Altimeter / recovery • Cameras
Credit: Richard Osborne
‘GoPro.com’ video cameras
Payloads (3)Credit: Richard Osborne
Examples of HPR
AspireSpace, ASRV-1aThetford1997K-class motor , 1250Ns2.1m long, 100mm diam.5000ft apogee
BURTBristol Uni Rocket Team1999NRC runner-up
2000Teams from • Manchester (UMIST)• Kent• Kingston
M.A.R.S.
2000
USA
25,000ft, aUK record
‘Amateur’ rocketry
AspireSpace, Comer (Scotland) & Lincs2001, 2002
Garvey Aerospace www.garvspace.comMojave, USA, 2005
Flometrics / San Siego State Universitywww.flometrics.com Mojave, USA, 2005
Recap
1. How does HPR differ from model rocketry?2. Some design guidelines for HPR3. Something on payloads4. Examples of HPR
• Still images... Videos...HARDWARE!5. Amateur rocketry6. Who can help?
– www.ukra.org.uk
October 28th, 2021