Lessons from Surveyor 6: Hopping Spacecraft for Low-Cost Surface Mobility on Small Bodies Niko Romer, Art Chmielewski, Nathan Barba, Nathan Fulmer. March 5, 2019 IEEE 2019 Aerospace Conference Copyright 2019 California Institute of Technology. U.S. Government sponsorship acknowledged. ~90 km
~20km Total distance driven by Curiosity in 6.5 years on Mars.
jpl.nasa.gov ~90 km ~600 km ~20km
3 jpl.nasa.gov PlanetarySociety.com Why Hop?
• Great scientific value in characterizing multiple regions. • Travel farther, faster, and cheaper than rovers. • Two types of hops can be considered: – Mechanical – Propulsive
March 5, 2019 4 jpl.nasa.gov Hopping Categorized – Mechanical
Agency Mission S/C Year Destination
USSR Phobos 2 PROP-F 1988 Phobos
JAXA Hayabusa MINERVA 2005 Itokawa http://cyberneticzoo.com/walking- machines/1983-7-prop-fphobos- hopper-soviet/ JAXA/ Hayabusa 2 MINERVA- 2018 Ryugu JAXA DLR II/MASCOT
DLR Rosetta Philae 2015 Comet 67P
ESA NASA N/A Hedgehog In Many possible dev.
NASA/JPL-Caltech/Stanford March 5, 2019 5 jpl.nasa.gov Hopping Categorized – Propulsive
UMD/GSFC/NASA NASA/GRC • Chopper (Comet Hopper), NASA Goddard • Mars Geyser Hopper, NASA Glenn - Discovery Class Proposal for - Discovery mission concept launch in 2016
March 5, 2019 6 jpl.nasa.gov 7 jpl.nasa.gov Surveyor Program: • Seven Pre-Apollo robotic scouts. • Program ran from 1966-1968.
LEM
Astronaut Pete Conrad
Surveyor 7
8 jpl.nasa.gov NASA/JPL-Caltech Surveyor 6 (1967)
First (and only until October 2018) successful hop on the surface of another body. • Soft lander for Lunar Surface • Dry Mass – 300 kg • ~16kg of excess propellant not used during initial soft landing. • Engineers performed a ”hop experiment.” • 2.5 second fire of ACS thrusters. • Average thrust 1390 N at +7° pitch. • Rose 4 m vertically, and translated 2.5 m horizontally.
March 5, 2019 NASA/JPL-Caltech 9 jpl.nasa.gov Surveyor Model
5 Coast • We modeled a two-burn hop trajectory using a “Surveyor-like” 300 kg spacecraft. 4.5 �, • Surface curvature is ignored in this
4 model. • For both models in this study, ∆v is the 3.5 required initial velocity for a distance ∆s. 3 Δ�% Δ�& #!'( 2.5 Δ� = Δ� + Δ� = 2 !"!#$ % & ()*&+ 2 α Δ� � − gravity Δ� − initial burn 1.5 Δ� − distance of hop Δ� − Retrobraking burn 1 � − launch angle -2 -1.5 -1 -0.5 0 0.5 1 1.5 2
March 5, 2019 10 jpl.nasa.gov Jump and Wait – An alternative hopping method
• This method involves rising to an altitude h and waiting for the planet or body to rotate underneath the spacecraft.
• Jump and Wait can save some fuel on fast-rotating bodies with low gravity.
" '(## Δ� = 2 ! !"!#$ -.()*/
�! − gravity � − mean radius of body Fulmer, 2017
� − polar angle �", �# − moment arms from Δ� − distance of hop rotational axis � − angular rate of rotation ℎ − maximum altitude
March 5, 2019 11 jpl.nasa.gov Comparing Jump-and-wait with Hopping
Example: Hopping on Ceres To determine when Jump and wait will save fuel on the equator: Jump and Wait becomes more efficient $ & ∆ % < %