AER11002 Spacecraft Design Tutorial

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Questions and Answers

A spacecraft executes a Hohmann transfer between two coplanar circular orbits. Assuming impulsive maneuvers and negligible atmospheric drag, which of the following statements regarding the velocity changes ($\Delta V$) and orbital geometry is most accurate?

  • The first impulse increases the spacecraft's kinetic energy, placing it into an elliptical transfer orbit with a semi-major axis equal to the arithmetic mean of the initial and final circular orbit radii; the geometry is independent of the central body's gravitational parameter.
  • The Hohmann transfer is optimal in terms of $\Delta V$ for any transfer angle between the initial and final orbits, always utilizing an elliptical transfer orbit regardless of the phasing between the departure and arrival points.
  • The transfer orbit's apoapsis coincides with the radius of the outer circular orbit, and the periapsis coincides with the radius of the inner circular orbit; the total $\Delta V$ is solely dependent on the ratio of the initial and final orbital radii and is minimized when the ratio approaches unity. (correct)
  • The Hohmann transfer involves two velocity impulses: the first at the initial orbit to increase the spacecraft's total energy, and a second at the target orbit to circularize the orbit, both minimizing fuel consumption regardless of transfer time.

A single-stage rocket launcher with a dry mass of 80,000 kg has a fuel mass of 600,000 kg and an exhaust velocity of 4,300 m/s. Assuming the required $\Delta V$ to reach orbit is 9,000 m/s, and neglecting gravity losses and atmospheric drag, what is the maximum payload mass the rocket can deliver to orbit, and how does the inclusion of gravity losses typically affect this calculation?

  • Payload mass: 4,395 kg; Gravity losses would increase the required $\Delta V$ to achieve orbit, thereby reducing the maximum payload mass. (correct)
  • Payload mass: 0 kg; The rocket cannot deliver any payload to orbit given the specified parameters and the influence of gravity losses.
  • Payload mass: 4,395 kg; Gravity losses would decrease the effective $\Delta V$ and thus increase the maximum payload mass delivered to orbit.
  • Payload mass: 10,000 kg; Gravity losses have a negligible impact on the payload calculation due to the high exhaust velocity.

A two-stage-to-orbit rocket launcher has an initial mass of 800,000 kg. The total required $\Delta V$ to reach orbit is 9,250 m/s, with the first stage providing a $\Delta V$ of 4,750 m/s. The exhaust velocity is 4,500 m/s for both stages, and the mass of the empty tank ejected after the first stage is 55,000 kg. Compared to a single-stage-to-orbit rocket with the same initial mass, total $\Delta V$, and exhaust velocity, assess the propellant mass requirements and discuss the primary advantage of using staging in this scenario.

  • Two-stage propellant mass: 662,816 kg; Single-stage propellant mass: 697,580 kg. Staging allows for the use of lower specific impulse engines on the first stage, optimizing thrust-to-weight ratios during initial ascent phases.
  • Two-stage propellant mass: 662,816 kg; Single-stage propellant mass: 697,580 kg. Staging increases structural efficiency, substantially reducing propellant requirements compared to a single-stage approach, enabling significantly higher payload fractions. (correct)
  • Two-stage propellant mass: 700,000 kg; Single-stage propellant mass: 650,000 kg. Staging reduces complexity and operational costs, proving advantageous despite marginal increases in propellant consumption due to increased engine restarts.
  • Two-stage propellant mass: 600,000 kg; Single-stage propellant mass: 750,000 kg. Staging improves reliability as there are multiple engines that can compensate for failures, outweighing the additional mass fraction due to staging.

A geostationary satellite is placed in a circular orbit around Earth. Given Earth's mass ($5.972 \times 10^{24}$ kg), the universal gravitational constant ($6.67 \times 10^{-11} Nm^2/kg^2$), and Earth's radius (6,371 km), at what altitude above Earth's surface must the satellite be positioned to maintain geostationary orbit, and what is its orbital speed, considering the effects of third-body perturbations from the Moon and Sun?

<p>Altitude: 35,861 km; Orbital speed: 3,071 m/s. Third-body perturbations will cause significant long-term variations in both the inclination and eccentricity of the orbit, requiring periodic station-keeping maneuvers. (D)</p>
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A satellite is in an elliptical orbit around Earth with a perigee altitude of 400 km and an apogee altitude of 4,000 km above the surface. Given Earth's mass ($5.972 \times 10^{24}$ kg), the universal gravitational constant ($6.67 \times 10^{-11} Nm^2/kg^2$), and Earth's radius (6,371 km), calculate the initial orbital period. If the orbital period is then increased by exactly 3 hours while maintaining the same ratio between perigee and apogee altitudes, what are the new perigee and apogee altitudes, considering the long-term effects of atmospheric drag?

<p>Initial period: 7.9 × 10³ s; New perigee altitude: 7.61 × 10⁵ m; New apogee altitude: 7.61 × 10⁶ m. Atmospheric drag will circularize the orbit over time, reducing both apogee and perigee altitudes, requiring periodic orbit boosts. (C)</p>
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A deep-space probe is designed to perform a flyby of Jupiter. The mission planners are considering using a gravity assist maneuver to alter the probe's trajectory and increase its speed significantly. Given Jupiter's mass ($1.898 \times 10^{27}$ kg) and the probe's initial velocity relative to Jupiter, derive the maximum possible velocity increase the probe could achieve and under what conditions this maximum is realized, taking into account the effects of Jupiter's atmospheric drag if the probe enters the upper atmosphere.

<p>The maximum velocity increase is achieved when the probe passes directly behind Jupiter, experiencing a 180-degree turning angle. Atmospheric drag must be carefully managed by accurate trajectory planning to avoid significant energy loss, which can negate the gravity assist benefit. (D)</p>
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A satellite is equipped with an electric propulsion system that provides a constant thrust. Describe how the continuous, low-thrust acceleration affects the satellite's orbital elements over time, specifically focusing on the changes in semi-major axis, eccentricity, and inclination, while considering the perturbative effects of solar radiation pressure and Earth's oblateness.

<p>Constant thrust causes a continuous spiral trajectory, predominantly affecting the semi-major axis, with smaller effects on eccentricity and inclination that depend on the thrust vector's orientation relative to the orbital plane. Solar radiation pressure and Earth's oblateness cause periodic variations in all orbital elements, requiring active control to maintain the desired orbit. (D)</p>
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A mission to Mars requires precise targeting for landing a rover on the surface. Discuss how uncertainties in the Mars atmosphere (density variations, winds), spacecraft navigation, and the deployment of a parachute affect the accuracy and precision of the landing, incorporating the use of advanced control systems to mitigate these uncertainties during the terminal descent phase.

<p>All three factors—atmospheric uncertainties, navigation errors, and parachute deployment variations—contribute substantially to landing dispersion. Advanced control systems using onboard sensors (e.g., Doppler radar, inertial measurement units) and algorithms enable real-time adjustments to the trajectory and parachute deployment, minimizing landing errors to within acceptable mission tolerances. (A)</p>
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A spacecraft is tasked with collecting samples from an asteroid's surface. Formulate a strategy for trajectory design that accounts for the asteroid's irregular shape, gravity field, and rotation, as well as the need to maintain stable orbits or trajectories around the asteroid to allow for precise sample collection, while considering non-gravitational forces such as solar radiation pressure.

<p>The spacecraft must map the asteroid's shape and gravity field extensively before designing stable 'terminator orbits' or hovering points that balance gravitational and centrifugal forces. Trajectory corrections must account for solar radiation pressure and any outgassing from the asteroid during approach and sample retrieval. (B)</p>
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A large space station in low Earth orbit (LEO) is subject to long-term atmospheric drag. Analyze the effects of this drag on the station's orbit, including changes in orbital altitude, period, and eccentricity, and evaluate various strategies for orbit maintenance, such as periodic reboosts using onboard thrusters or the deployment of a drag-compensation system, incorporating the impact of solar activity on atmospheric density.

<p>Atmospheric drag causes a gradual decrease in altitude and period while tending to circularize the orbit over time. Orbit maintenance strategies include periodic reboosts and drag compensation systems. Solar activity significantly influences atmospheric density, affecting the frequency and magnitude of required reboosts. (C)</p>
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A CubeSat is deployed into a highly elliptical Earth orbit (HEO). Assess the impact of perturbations from the Moon, Sun, and Earth's oblateness on the CubeSat's long-term orbital stability, and propose a control strategy to mitigate these effects while considering the limited resources (power, propellant) available on a CubeSat platform.

<p>All three perturbations significantly degrade the orbit: the Moon inducing inclination changes, the Sun causing eccentricity variations, and the oblateness affecting the argument of perigee. A cost-effective strategy involves a combination of passive gravity-gradient stabilization and infrequent, strategically timed micro-propulsion maneuvers triggered by onboard sensors. (D)</p>
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For an interplanetary mission, such as a mission to Europa, compare and contrast the use of chemical propulsion, solar electric propulsion (SEP), and nuclear thermal propulsion (NTP) in terms of mission duration, propellant requirements, payload capacity, and overall mission complexity, taking into account the radiation environment around Jupiter and the limitations it imposes on the spacecraft's components.

<p>Chemical propulsion enables fast transfers but demands substantial propellant. SEP offers high specific impulse, reducing propellant needs but increasing transit times; radiation degradation is a serious concern near Jupiter. NTP presents a high thrust-to-weight ratio, enabling shorter transit times than SEP, yet its complexity and the radiation environment remain significant challenges. (C)</p>
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Develop a closed-loop control system architecture for a spacecraft performing autonomous rendezvous and docking with a target satellite in geostationary orbit (GEO). Describe the necessary sensors (e.g., GPS, star trackers, lidar), actuators (e.g., reaction wheels, thrusters), and algorithms (e.g., Kalman filters, model predictive control) to achieve high precision and reliability, especially during the terminal phase, while accounting for GEO's unique challenges (通信延迟,limited GPS availability, 地球反照率的影响).

<p>The control system requires high-accuracy GPS and star trackers for initial orbit determination, transitioning to lidar and vision-based navigation for terminal approach. An Extended Kalman Filter integrates sensor data, while model predictive control commands thrusters that compensate for GEO's perturbations. Communications delays are mitigated using predictive algorithms; Earth albedo is accounted for by advanced image processing. (B)</p>
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Design a thermal management system for a spacecraft destined for a mission to Venus. Analyze the significant challenges posed by Venus's high surface temperature and dense atmosphere, and evaluate different thermal control techniques, such as multi-layer insulation (MLI), heat pipes, radiators, and phase-change materials (PCMs), to maintain the spacecraft's internal components within acceptable temperature ranges, while minimizing weight and power consumption.

<p>The thermal design will consist of MLI to insulate internal components, heat pipes to transport heat to internal radiators situated away from direct solar radiation, and carefully selected PCMs to buffer thermal transients. Radiator capacity is optimized. Weight and power budgets are carefully considered to maximize the system’s efficiency and longevity. (B)</p>
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Assess the feasibility and implications of constructing a large-scale solar power satellite (SPS) in geostationary orbit (GEO) to wirelessly transmit energy to Earth. Analyze the technical challenges related to orbital assembly, microwave or laser power transmission efficiency, atmospheric effects, potential impacts on the GEO environment (e.g., space debris, radio frequency interference), safety concerns, and economic viability compared to terrestrial renewable energy sources.

<p>Large-scale SPS deployment is technically feasible but economically prohibitive and poses significant environmental risks. Assembled in orbit using robotic systems, the long-term reliability, maintenance, and efficiency of the wireless power beaming technology as well as the high potential for interference from radio signals, make it a less viable technology compared to terrestrial renewable energy sources. (B)</p>
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Consider a scenario in which a spacecraft must perform an emergency collision avoidance maneuver due to a potential impact with a piece of space debris. Given the limitations in onboard propellant, sensor accuracy, and computation time, formulate an optimal trajectory planning strategy to minimize the probability of collision while minimizing the $\Delta V$ expenditure, taking into account the uncertainties in the debris's orbital parameters and the spacecraft's own position and velocity.

<p>The strategy must involve a sequence of small, carefully timed maneuvers to maximize the change in the spacecraft's trajectory while minimizing overall $\Delta V$. Sensor inaccuracies are modeled with probabilistic methods (e.g., Kalman filters), and trajectory planning incorporates stochastic optimization techniques to account for uncertainties in debris parameters. (A)</p>
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A constellation of small satellites is designed to provide global internet coverage. Analyze the trade-offs between different orbital altitudes (LEO, MEO) and constellation architectures (Walker, Iridium-like) in terms of coverage area, signal latency, power requirements, inter-satellite links, atmospheric drag, radiation exposure, and the cost of deployment and maintenance, while maximizing internet bandwidth and minimizing signal interference.

<p>An optimal design balances altitude and configuration trade-offs. A LEO constellation minimizes latency but faces high drag and smaller coverage, while MEO extends coverage and reduces drag but at higher cost and latency. Inter-satellite links augment coverage and capacity, but increase complexity and power needs. (D)</p>
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A spacecraft is equipped with an ion thruster that operates at a very high specific impulse but produces a low thrust force. Formulate an optimal control strategy for guiding the spacecraft from a low Earth orbit (LEO) to a geostationary transfer orbit (GTO) using continuous low-thrust propulsion. The strategy should account for Earth's oblateness, solar radiation pressure, and the ion thruster's limited throttling range, while minimizing the total transfer time and propellant consumption.

<p>Trajectory design should leverage resonant orbit transfers, synchronizing thrust arcs with perigee passages to minimize fuel consumption while actively managing the spacecraft's attitude to counteract disturbances induced by thrust steering. (B)</p>
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Explain the influence of relativistic effects, specifically time dilation and the Shapiro delay, on deep-space navigation and communication, especially during missions involving high-precision ranging and telemetry with distant spacecraft near massive celestial bodies (e.g., the Sun, Jupiter). Furthermore, how does one compensate for these effects in mission planning and real-time operations to ensure accurate positioning and data transmission?

<p>Relativistic phenomena are incorporated into models using sophisticated mathematical frameworks and computational techniques, which allows real-time corrections to both navigation data and communication signals. Time dilation and Shapiro delays are most pronounced when signals pass close to massive bodies and must be accounted for to maintain navigational precision. (D)</p>
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Flashcards

Hohmann Transfer

A maneuver used to transfer a spacecraft between two circular orbits of different altitudes using two engine impulses.

Rocket Equation

ΔV = vex * ln(mo/mf), where ΔV is the change in velocity, vex is the exhaust velocity, mo is the initial mass, and mf is the final mass.

Kepler's Third Law

τ² = (4π²/GM) * a³, where τ is the orbital period, G is the gravitational constant, M is the mass of the central body, and a is the semi-major axis.

Newton's Law of Gravity

F = (Gm1m2) / r², where F is the gravitational force, G is the gravitational constant, m1 and m2 are the masses of the two objects, and r is the distance between their centers.

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Geostationary orbit

An orbit where a satellite appears stationary with respect to a point on Earth.

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Perigee

The point in an orbit that is closest to the Earth.

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Apogee

The point in an orbit that is farthest from the Earth.

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Study Notes

Spacecraft Tutorial Questions Overview

  • The tutorial questions are designed to help students learn and receive feedback
  • These questions will assess detailed understanding of spacecraft
  • The questions are similar to those in part B of the exam
  • The marks for each question indicate its worth in the exam
  • The exam format may differ from recent examples due to social distancing, but the content remains the same
  • Detailed exam information will be given during the first and second semesters
  • Past exam papers are available on MOLE

Descriptive/Explanation Question

  • Explain the Hohmann transfer between two circular orbits using a diagram
  • Include the geometry of the Hohmann transfer orbit

Useful Equations for Calculations

  • Rocket equation: ΔV = vex * ln(mo/mf)
  • Kepler's third law: τ² = (4π² / Gm₁) * a³
  • Newton's Law of Gravity: F = (Gm₁m₂) / r²

Calculation Problems

  • Problem 1: Find the maximum payload a single-stage rocket launcher can carry into orbit, given:
    • Dry mass (excluding payload): 80,000kg
    • Required ΔV: 9,000m/s
    • Exhaust velocity: 4,300m/s
    • Available fuel mass: 600,000kg
  • Problem 2: Consider a two-stage-to-orbit rocket launcher, given:
    • Initial mass: 800,000kg
    • Total required ΔV: 9,250m/s
    • First stage ΔV: 4,750m/s
    • Exhaust velocity (both stages): 4,500m/s
    • Empty tank mass ejected at end of first stage: 55,000kg
    • Calculate the total mass of propellant used and compare it to the mass of propellant for a single-stage-to-orbit rocket
  • Problem 3: A geostationary satellite orbits at a fixed position relative to Earth, given:
    • Mass of the Earth: 5.972 × 10²⁴kg
    • Universal constant of gravitation: 6.67 × 10⁻¹¹ Nm²/kg²
    • Radius of the Earth: 6,371km
    • Determine the height above Earth's surface and the satellite's orbital speed
  • Problem 4: A satellite in an elliptical orbit around Earth has:
    • Perigee: 400km above the surface
    • Apogee: 4,000km above the surface
    • Calculate the orbital period
    • Determine the perigee and apogee if the orbital period is increased by 3 hours, maintaining the same ratio between the two
    • Use:
      • Mass of the Earth: 5.972 × 10²⁴kg
      • Universal constant of gravitation: 6.67 × 10⁻¹¹ Nm²/kg²
      • Radius of the Earth: 6,371km

Numerical Solutions

  • Problem 1: 4,395kg
  • Problem 2:
    • 2-stage-to-orbit: 662,816kg
    • single-stage-to-orbit: 697,580kg
  • Problem 3: 35,861km; 3,071m/s
  • Problem 4:
    • 7.9 × 10³s
    • new perigee = 7.61 × 10⁵m
    • new apogee = 7.61 × 10⁶m

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