Mass Driver PDR

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Mass Driver PDR February 25, 2020

Transcript of Mass Driver PDR

Page 1: Mass Driver PDR

Mass Driver PDRFebruary 25, 2020

Page 2: Mass Driver PDR

Mission Profile (Mars → Phobos)

● Launch windows are defined by phobos

position and tether sling spin up time

○ Phobos must be -29.033° from

Olympus Mons (right ascension)

○ Max turnover = 3 launches/sol

● Acceleration Profile

○ 4.77 km/s Launch Velocity

○ 4.47 km/s Velocity past

atmosphere

○ 2 G’s net

● Total Orbital Flight Time 14.69 hrs

Page 3: Mass Driver PDR

Orbital Trajectory

ΔV (km/s) Time (hrs)

Launch 4.77 6.17

Burn 1 0.286 8.52

Burn 2 0.375 RNDVZ

Total 0.661 14.69

Page 4: Mass Driver PDR

Considerations & Deviations

● Acceleration modification

○ Make time and distance shorter

○ Launch Velocity includes drag and rotation

● Orbital analysis

○ No perturbations

○ No eccentricity/inclinations

● Risk Assessment

○ If launch fails, more ΔV is required

○ If burn 1 fails, the taxi will return to Olympus Mons

○ If burn 2 fails, no return possibility without significant ΔV

Page 5: Mass Driver PDR

Current Mass Driver Design

MagLev System

• Proven to handle loads of our magnitude (passenger trains)

• Allows us to more easily decelerate the cradle for reusability

• Located at the base of Olympus Mons

• Using Null-Flux Coils for Repulsive Levitation

Page 6: Mass Driver PDR

Current Mass Driver Design

Important Parameters

• Track Length: 635 km

• Launch Duration: 4 minutes 14 seconds

• 2g constant acceleration

• F required,propulsion = 6.49 MN

• F required,levitation = 1.1 MN

Page 7: Mass Driver PDR

Candidate Systems

- Propellant saved: 477 Mg

PropulsionForce required: 6.49 MN

Railgun

LevitationForce required: 1.11 MN

Coilgun Maglev

Linear Synchronous

Motor (LSM)

Linear Induction

Motor (LIM)

Wheels Suspended

Electromagnetic

Suspension (EMS)

Electrodynamic

Suspension (EDS)

Page 8: Mass Driver PDR

Mass Driver Technology

z

x

Page 9: Mass Driver PDR

Linear Induction Controller

• Set velocity that is needed to escape Mars(5.03

km/s) Moon(2.38 km/s)

• Sense the velocity of the taxi vs how fast it needs to

have been going

• Increase the current through the LIM to increase

acceleration to needed levels

Journal of Transportation

Force will increase linearly with an

increase in current

Page 10: Mass Driver PDR

Martian Taxi Catching SystemCradle

Information

Mass 100 tons

Material Aluminum 6061

T6

Length 25 meters

Magnet Width 15 meters

Width 36 meters

Page 11: Mass Driver PDR

Mass Driver Materials & Structural Analysis

Mass Driver

Parts

Materials

Rail (EDS system) Iron, Wrought or

Rhenium beams

Vacuum Casing Iron, Wrought

Magnets 15 Lanthanides

Scandium

Yttrium

Niobium Titanium

Structural Integrity Precautions for

Track

• Rounded edges to prevent

cracking

• FEA testing will be conducted

through multiple scenarios (G-

forces, heat, cooldown etc.).

Suggestions needed to increase

reliability.

Page 12: Mass Driver PDR

Power Consumption

Mars The Moon

Peak Power

Consumption (GW)

30.1 13.5

Average Power

Consumption (GW)

14 6.6

Total Energy

Consumption (GJ)

3600 830

● Power consumption peaks at the Taxis top speed when drag force is at a maximum

● Power is stored in batteries and used when solar panels can no longer keep up with the

required power

● VVVF (Variable Voltage, Variable Frequency) power is provided to support the needs of

the MagLev

Page 13: Mass Driver PDR

Power Production and Storage

Mars The Moon

Solar Panel Power (MW) 100 10

Solar Panel Area (km2) .56 .024

Total Mass (Mg) 5500 1100

● Solar Panels provide limited energy and

charge the batteries over the long

duration between sets of launches

● Batteries are capable of holding enough

energy to launch 3 Taxis consecutively

Page 14: Mass Driver PDR

Human Considerations

Forward Acceleration

Backwards Acceleration

7G’s absolute max acceleration (at any given time), 2G’s max sustained

acceleration recommended

Page 15: Mass Driver PDR

Mass Driver Thermal Management• Power Consumption: 30 MW that

needs to be dissipated via Heat

Sinks.

• Due to the amount of heat

generated, the rail will slowly

erode over time, so it has to be

liquid cooled.[1]

Thermal

Systems

(Mars)

Mass Volume Power

Heat Sinks 6.49 Mg 34,285.7

m3

Passive

Cooling

Liquid

Cooling for

the Rail

172.8 Mg 5.1 * 108

m3

230 MW

1. M. Johnson, P. Cote, F. Campo and P. Vottis, "Railgun Erosion Simulator," 2005 IEEE Pulsed Power Conference,

Monterey, CA, 2005, pp. 245-248.

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Analysis of Aerodynamic Drag

Aerodynamic Effects

• Max Drag is around 53kN of

force

• Aerodynamic heating is 3.14

GW which would be less than

re-entry heating

• Further analysis is required

based on keeping the magnets

supercooled