This document provides a summary of a satellite constellation design project to monitor the US-Mexico border. The constellation aims to provide near-continuous surveillance coverage of the border region using a minimum of 16 satellites. Key aspects of the design include:
- Choosing a sun-synchronous low Earth orbit with 15.9 revolutions per day to provide adequate coverage.
- Selecting a multi-spectral mid-IR imaging payload to achieve 1m ground resolution between 0.4-4μm wavelengths.
- Designing a 373GB data storage and 424Mbps downlink capability to transmit imagery to a ground station.
- Sizing solar panels and batteries to power the 541W system during
This document outlines the design of a satellite constellation to monitor the US-Mexico border. The constellation will consist of 16 satellites in low Earth orbit with an orbital period of 15.93 revolutions per day. Each satellite will carry an imaging payload with 1m resolution to collect data on potential threats along the border. The total cost of developing, launching and operating the constellation is estimated to be $498.7 million, meeting the budget constraint of less than $500 million. The constellation is designed to provide continuous coverage of the border region with gaps of no more than 12 minutes.
The KMEC mission involves sending two spacecraft to Saturn over 6 years to study cosmic dust, ultraviolet imaging, and space recognition between the payloads. Each spacecraft is octagonal and 6m tall, made of aluminum. The 100kg payload includes dust, UV, and ranging instruments. A chemical propulsion system will perform orbital maneuvers. Power comes from an RTG and backup battery. Thermal control uses an RTG and radiator. The spacecraft structure is sized to withstand launch stresses and the environment at Saturn.
The mission aims to map space debris in low Earth orbit between 1,000-3,000 km using 6 small satellites. Each satellite will use an infrared camera to image debris and calculate its orbit. The satellites will be placed in 3 evenly spaced orbital planes by a Delta II rocket and slowly lower their orbits over 30 days to map the entire region. Their design emphasizes modularity for low cost and mass, using commercial off-the-shelf components, with a focus on thermal control, power, communications and orbital maneuvering systems to complete the debris mapping mission.
The document provides solutions to problems related to satellite systems and components. It includes:
1) Calculations of telemetry frame transmission time, maximum propagation delay, and solar cell efficiencies for a geostationary communications satellite.
2) Estimates of the area, height, and power output of solar cells on a spinner satellite.
3) Calculations of the size and area of solar sails or cells needed to power different geostationary satellite designs.
4) Determinations of battery capacity and weight for a direct broadcast TV satellite.
5) Calculations of antenna diameters, beamwidths, and gains for satellites using Ku and Ka band frequencies.
6) Estimates of antenna dimensions and
This document discusses orbital mechanics concepts including:
1) Calculating orbital parameters like velocity and period for satellites in circular orbits between 322-1400 km altitude.
2) Designing an observation satellite orbit with a 4 hour period to pass directly over a ground station every 4 hours at an elevation angle above 10 degrees.
3) Computing the true anomaly of a satellite in an elliptical orbit with eccentricity 0.15 and semi-major axis of 9000 km at a height of 2000 km.
4) Determining the velocities of satellites in both circular and elliptical orbits at the same orbital radius.
5) Relating the orbital periods of two satellites with semi-major axes of 18000 km
The document provides an overview of metric and scientific units used in astronomy, including prefixes, fundamental SI units of length, mass, and time. It lists several special units used to measure large astronomical distances and objects, such as astronomical units, light-years, and parsecs. It also gives examples of metric equivalents for units like years, kilograms, and seconds. Finally, it mentions two resources that demonstrate relative sizes of objects in the universe on a scale of powers of ten.
This document summarizes how GPS systems use linear algebra to determine location. It explains that GPS uses at least 3 satellites to triangulate a receiver's position via trilateration. The satellites transmit their location and arrival time. This creates a system of equations relating distance from each satellite equal to the difference between signal transmission and receipt times. Linear algebra is then used to solve the system of equations, determining the receiver's x, y, z coordinates. The process involves constructing matrices from the satellite data and time differences, then reducing them to their row echelon form to solve for position.
Remote sensing platforms can be ground-based, airplane-based, or satellite-based. Satellite platforms can be in sun-synchronous polar orbits for global coverage, non-sun-synchronous orbits for variable coverage, or geostationary orbits for continuous regional coverage. Remote sensing can be passive using sunlight or active using its own energy source like radar or lidar. Spatial, spectral, radiometric, and temporal resolutions provide information on a sensor's ability to distinguish locations, wavelengths, brightness values, and revisit times. Raster data formats represent imagery as a grid of pixels organized into rows, columns, and bands.
This document outlines the design of a satellite constellation to monitor the US-Mexico border. The constellation will consist of 16 satellites in low Earth orbit with an orbital period of 15.93 revolutions per day. Each satellite will carry an imaging payload with 1m resolution to collect data on potential threats along the border. The total cost of developing, launching and operating the constellation is estimated to be $498.7 million, meeting the budget constraint of less than $500 million. The constellation is designed to provide continuous coverage of the border region with gaps of no more than 12 minutes.
The KMEC mission involves sending two spacecraft to Saturn over 6 years to study cosmic dust, ultraviolet imaging, and space recognition between the payloads. Each spacecraft is octagonal and 6m tall, made of aluminum. The 100kg payload includes dust, UV, and ranging instruments. A chemical propulsion system will perform orbital maneuvers. Power comes from an RTG and backup battery. Thermal control uses an RTG and radiator. The spacecraft structure is sized to withstand launch stresses and the environment at Saturn.
The mission aims to map space debris in low Earth orbit between 1,000-3,000 km using 6 small satellites. Each satellite will use an infrared camera to image debris and calculate its orbit. The satellites will be placed in 3 evenly spaced orbital planes by a Delta II rocket and slowly lower their orbits over 30 days to map the entire region. Their design emphasizes modularity for low cost and mass, using commercial off-the-shelf components, with a focus on thermal control, power, communications and orbital maneuvering systems to complete the debris mapping mission.
The document provides solutions to problems related to satellite systems and components. It includes:
1) Calculations of telemetry frame transmission time, maximum propagation delay, and solar cell efficiencies for a geostationary communications satellite.
2) Estimates of the area, height, and power output of solar cells on a spinner satellite.
3) Calculations of the size and area of solar sails or cells needed to power different geostationary satellite designs.
4) Determinations of battery capacity and weight for a direct broadcast TV satellite.
5) Calculations of antenna diameters, beamwidths, and gains for satellites using Ku and Ka band frequencies.
6) Estimates of antenna dimensions and
This document discusses orbital mechanics concepts including:
1) Calculating orbital parameters like velocity and period for satellites in circular orbits between 322-1400 km altitude.
2) Designing an observation satellite orbit with a 4 hour period to pass directly over a ground station every 4 hours at an elevation angle above 10 degrees.
3) Computing the true anomaly of a satellite in an elliptical orbit with eccentricity 0.15 and semi-major axis of 9000 km at a height of 2000 km.
4) Determining the velocities of satellites in both circular and elliptical orbits at the same orbital radius.
5) Relating the orbital periods of two satellites with semi-major axes of 18000 km
The document provides an overview of metric and scientific units used in astronomy, including prefixes, fundamental SI units of length, mass, and time. It lists several special units used to measure large astronomical distances and objects, such as astronomical units, light-years, and parsecs. It also gives examples of metric equivalents for units like years, kilograms, and seconds. Finally, it mentions two resources that demonstrate relative sizes of objects in the universe on a scale of powers of ten.
This document summarizes how GPS systems use linear algebra to determine location. It explains that GPS uses at least 3 satellites to triangulate a receiver's position via trilateration. The satellites transmit their location and arrival time. This creates a system of equations relating distance from each satellite equal to the difference between signal transmission and receipt times. Linear algebra is then used to solve the system of equations, determining the receiver's x, y, z coordinates. The process involves constructing matrices from the satellite data and time differences, then reducing them to their row echelon form to solve for position.
Remote sensing platforms can be ground-based, airplane-based, or satellite-based. Satellite platforms can be in sun-synchronous polar orbits for global coverage, non-sun-synchronous orbits for variable coverage, or geostationary orbits for continuous regional coverage. Remote sensing can be passive using sunlight or active using its own energy source like radar or lidar. Spatial, spectral, radiometric, and temporal resolutions provide information on a sensor's ability to distinguish locations, wavelengths, brightness values, and revisit times. Raster data formats represent imagery as a grid of pixels organized into rows, columns, and bands.
1) The document summarizes recent measurements of pulsar masses, finding 35 precision measurements including some with masses over 1.8 solar masses.
2) It discusses possible formation scenarios for eccentric millisecond pulsars that could provide constraints on neutron star structure if their masses are measured precisely.
3) The mass distribution of millisecond pulsars is likely bimodal rather than normal, with peaks at 1.4 and 1.8 solar masses, implying more massive pulsars are common than previously thought.
This document provides a preliminary study for the AROSAT satellite system. It discusses several key requirements including coverage area, resolution capabilities, duty cycle, onboard storage and download rates. It evaluates three potential spacecraft configurations and their impact on drag, solar array effectiveness and risk. Configuration #2 is preferred as it minimizes drag while having a simple solar array design. The document also examines how spacecraft altitude affects optical instrument parameters and the propulsion systems needed to compensate for atmospheric drag at different altitudes. Electric propulsion is recommended to enable lower orbits. Overall architectures are proposed for Configuration #2 that could meet requirements.
This document contains solutions to 5 questions about orbital mechanics. Question 1 calculates the centripetal and centrifugal accelerations, velocity, and orbital period of a satellite in a 1,400 km circular orbit. Question 2 does similar calculations for a 322 km circular orbit, finding the orbital angular velocity, period, and velocity. Question 3 calculates Doppler shifts for signals from this satellite received by observers in space and on the Earth's surface. Question 4 states Kepler's laws of planetary motion and uses the third law to find the orbital period of a satellite in an elliptical orbit with a 39,152 km apogee and 500 km perigee.
The document provides information about several astronomical objects and phenomena including:
- The Sombrero Galaxy and NGC 1300, examples of different types of spiral galaxies.
- Hoag's Object, an example of a ring galaxy.
- Kepler's Supernova Remnant captured using Chandra X-ray Observatory.
- Infrared image and details about the Milky Way galaxy such as size, number of stars, and rotation period.
- Technical specifications and images of Hubble Space Telescope, Chandra X-ray Observatory, and their instruments.
This document discusses the concept of an X-ray interferometer called MAXIM that could achieve micro-arcsecond resolution. It would consist of an optics spacecraft holding multiple flat mirrors in formation with a detector spacecraft to form interference patterns. The goal is to image phenomena like black hole accretion disks and supernovae with much higher resolution than current telescopes. A pathfinder mission is proposed with 100 microarcsecond resolution using two spacecraft separated by 1.4 meters as a technology demonstration.
The researchers investigate atmospheric evaporation of four super-Earth exoplanets - HD 97658 b, GJ 1214 b, 55 Cnc e, and CoRoT-7 b - using X-ray observations of the host stars to estimate planetary mass loss over time. They find the planets receiving the greatest amount of high-energy stellar radiation, like CoRoT-7 b, have likely experienced significant atmospheric mass loss and may be sculpted into lower mass, denser remnant cores. The estimated current mass loss rates and total integrated mass lost over the star's lifetime support this hypothesis.
The document discusses using astrometric observations of Jupiter's Galilean moons to determine their orbital properties and masses. The goals were to precisely measure the orbital periods and radii of Io, Europa, Ganymede, and Callisto using telescope images over multiple nights. Periodic regression analysis of the moon positions yielded accurate periods within 0.05% but less precise radii. While Kepler's laws allowed mass calculations, the results were off by orders of magnitude due to limitations of the data. More observations would be needed to precisely determine moon masses through astrometry alone.
This document discusses satellite orbits and positioning systems. It begins by introducing satellite system components like subsystems, uplinks and downlinks. It then defines key terms related to satellite orbits, such as the minimum velocity needed to orbit Earth and different orbit classifications like LEO, MEO, HEO and polar orbits. Multiple access methods for satellites like TDMA, FDMA and CDMA are also covered. The document concludes by providing an overview of the GPS system and its space, control and user segments.
This document summarizes Tyler Croteau's proposed CubeSat mission for studying electromagnetic ion cyclotron (EMIC) waves using a constellation of 6 miniaturized 0.5U CubeSats. The primary objective is to conduct multipoint measurements of EMIC waves at high latitudes using a boom-deployed magnetometer on each CubeSat. Each 0.5U CubeSat would be less than 650g and utilize solar cells and lithium-ion batteries for power. The CubeSats would be deployed in a string-of-pearls formation from a P-POD launcher into a low Earth orbit for coordinated science measurements over multiple years. Attitude control would rely on passive gravity
This document discusses non-radioisotope power systems for solar system exploration missions without access to sunlight. It mentions using plutonium-238, lithium, sulfur hexafluoride, aluminum, water, magnesium, and carbon dioxide in potential power systems. It also summarizes the science goals and expected data collection of the ALIVE Venus lander mission, including instruments to measure atmospheric structure, composition, and meteorology and collect descent imagery and panoramic photos.
This document discusses using shepherd satellites to provide guidance, navigation, and control for arrays of microsatellites performing formation flying. It proposes using optical scattering and gradient forces generated by lasers on the shepherd satellites to apply corrective forces to the microsatellite array from a distance. Analytic models predict these radiation forces could provide restorative forces of 10-5 N to 10-4 N using laser powers of 10-10 kW to 100 kW. Potential applications include drag makeup for low Earth orbiting satellites, position control for array formation, and correcting perturbations in geosynchronous Earth orbit.
This document provides a design study for a proposed CubeSat mission called SWaRMM (Space Weather and Radiation Multi-point Magnetometry) that would deploy six 0.5U CubeSats in a slowly separating string to conduct multi-point magnetometer measurements. Each CubeSat would carry a single mini fluxgate magnetometer to characterize phenomena like EMIC waves and Birkeland currents. Preliminary designs for the CubeSats include a structure to carry solar panels and a payload boom, an electrical power system using solar cells and batteries, and attitude control possibly using gravity gradient and hysteresis rods. Initial analyses show the design could meet power and mass requirements to achieve the science goals of the low-cost
Simulation of Deployment and Operation of an Earth Observing SatelliteAlber Douglawi
1) A simulation was conducted of a spacecraft deploying from a launch vehicle and performing attitude control to point its sensor at targets on Earth. Initially, the spacecraft tumbled out of the launch vehicle and thrusters were used to detumble it and align with the local horizontal frame.
2) During operations, a targeting algorithm prioritized 1000 targets and reaction wheels oriented the spacecraft to point at the highest value targets within its sensor range every 100 seconds. Over one day, this allowed it to image 235 targets worth a total of $67461.
3) Disturbance torques from the gravity gradient, solar radiation pressure, aerodynamics, and flexing of deployed solar panels and sensor were modeled. Gains
1) MagBeam is a proposed plasma propulsion system that uses focused plasma beams and magnetic fields to transfer power and thrust separately from spacecraft payloads, enabling fast, efficient propulsion for multiple space missions.
2) Laboratory experiments at the University of Washington have demonstrated the focusing and guiding of plasma beams over short distances using magnetic fields, with the goal of scaling this technology up for applications requiring kilometers of beam propagation.
3) Preliminary analyses suggest MagBeam could enable dramatic mass and cost savings over chemical propulsion for applications like transferring payloads to low Earth orbit, geosynchronous orbit, and missions to Mars through reusable, high-efficiency plasma thrusters.
This document summarizes a presentation about satellite communication. It discusses the basic concept of a communication satellite, how satellites are used as relay stations to transmit signals between Earth stations, and the different types of satellite orbits including geostationary, low Earth, and medium Earth orbits. It also covers topics like inter-satellite links, routing between satellites, common modulation techniques, and recent developments in satellite communication technology.
The document discusses spatial control of photons and optical vortices. It describes how photons can be put into Laguerre-Gaussian modes using mode converters or holograms. These modes carry orbital angular momentum and can be used to encode quantum information. Precise control over generation, manipulation, and measurement of photon states enables applications in quantum communication.
A dwarf galaxy is colliding with the large spiral galaxy NGC 1232, as revealed by X-ray observations from Chandra. The collision is creating a large region (7.25 kpc in diameter) of shocked, hot gas with a temperature of around 5.8 million kelvin. The X-ray luminosity of this collisional aftermath is estimated to be 3.7x10^38 ergs/s. Based on the size and temperature of the X-ray emitting region, the collision likely involves a dwarf galaxy and represents a massive energy input into NGC 1232, far exceeding a typical supernova. Such collisions detected solely in X-rays may provide insights into the role of dwarf galaxy interactions in the evolution of
New Post-DART Collision Period for the Didymos System: Evidence for Anomalous...Sérgio Sacani
On September 26, 2022, NASA’s DART spacecraft impacted Dimorphos, the secondary asteroid in
the (65803) Didymos system, so that the efficiency with which a satellite could divert an asteroid
could be measured from the change in the system’s period. We present new data from the Thacher
Observatory and measure a change in period, ∆P = −34.2 ± 0.1 min, which deviates from previous
measurements by 3.5 σ. This suggests that the system period may have decreased by ∼ 1 minute in
the 20 to 30 days between previous measurements and our measurements. We find that no mechanism
previously presented for this system can account for this large of a period change, and drag from impact
ejecta is an unlikely explanation. Further observations of the (65803) Didymos system are needed to
both confirm our result and to further understand this system post impact.
1) The document summarizes recent measurements of pulsar masses, finding 35 precision measurements including some with masses over 1.8 solar masses.
2) It discusses possible formation scenarios for eccentric millisecond pulsars that could provide constraints on neutron star structure if their masses are measured precisely.
3) The mass distribution of millisecond pulsars is likely bimodal rather than normal, with peaks at 1.4 and 1.8 solar masses, implying more massive pulsars are common than previously thought.
This document provides a preliminary study for the AROSAT satellite system. It discusses several key requirements including coverage area, resolution capabilities, duty cycle, onboard storage and download rates. It evaluates three potential spacecraft configurations and their impact on drag, solar array effectiveness and risk. Configuration #2 is preferred as it minimizes drag while having a simple solar array design. The document also examines how spacecraft altitude affects optical instrument parameters and the propulsion systems needed to compensate for atmospheric drag at different altitudes. Electric propulsion is recommended to enable lower orbits. Overall architectures are proposed for Configuration #2 that could meet requirements.
This document contains solutions to 5 questions about orbital mechanics. Question 1 calculates the centripetal and centrifugal accelerations, velocity, and orbital period of a satellite in a 1,400 km circular orbit. Question 2 does similar calculations for a 322 km circular orbit, finding the orbital angular velocity, period, and velocity. Question 3 calculates Doppler shifts for signals from this satellite received by observers in space and on the Earth's surface. Question 4 states Kepler's laws of planetary motion and uses the third law to find the orbital period of a satellite in an elliptical orbit with a 39,152 km apogee and 500 km perigee.
The document provides information about several astronomical objects and phenomena including:
- The Sombrero Galaxy and NGC 1300, examples of different types of spiral galaxies.
- Hoag's Object, an example of a ring galaxy.
- Kepler's Supernova Remnant captured using Chandra X-ray Observatory.
- Infrared image and details about the Milky Way galaxy such as size, number of stars, and rotation period.
- Technical specifications and images of Hubble Space Telescope, Chandra X-ray Observatory, and their instruments.
This document discusses the concept of an X-ray interferometer called MAXIM that could achieve micro-arcsecond resolution. It would consist of an optics spacecraft holding multiple flat mirrors in formation with a detector spacecraft to form interference patterns. The goal is to image phenomena like black hole accretion disks and supernovae with much higher resolution than current telescopes. A pathfinder mission is proposed with 100 microarcsecond resolution using two spacecraft separated by 1.4 meters as a technology demonstration.
The researchers investigate atmospheric evaporation of four super-Earth exoplanets - HD 97658 b, GJ 1214 b, 55 Cnc e, and CoRoT-7 b - using X-ray observations of the host stars to estimate planetary mass loss over time. They find the planets receiving the greatest amount of high-energy stellar radiation, like CoRoT-7 b, have likely experienced significant atmospheric mass loss and may be sculpted into lower mass, denser remnant cores. The estimated current mass loss rates and total integrated mass lost over the star's lifetime support this hypothesis.
The document discusses using astrometric observations of Jupiter's Galilean moons to determine their orbital properties and masses. The goals were to precisely measure the orbital periods and radii of Io, Europa, Ganymede, and Callisto using telescope images over multiple nights. Periodic regression analysis of the moon positions yielded accurate periods within 0.05% but less precise radii. While Kepler's laws allowed mass calculations, the results were off by orders of magnitude due to limitations of the data. More observations would be needed to precisely determine moon masses through astrometry alone.
This document discusses satellite orbits and positioning systems. It begins by introducing satellite system components like subsystems, uplinks and downlinks. It then defines key terms related to satellite orbits, such as the minimum velocity needed to orbit Earth and different orbit classifications like LEO, MEO, HEO and polar orbits. Multiple access methods for satellites like TDMA, FDMA and CDMA are also covered. The document concludes by providing an overview of the GPS system and its space, control and user segments.
This document summarizes Tyler Croteau's proposed CubeSat mission for studying electromagnetic ion cyclotron (EMIC) waves using a constellation of 6 miniaturized 0.5U CubeSats. The primary objective is to conduct multipoint measurements of EMIC waves at high latitudes using a boom-deployed magnetometer on each CubeSat. Each 0.5U CubeSat would be less than 650g and utilize solar cells and lithium-ion batteries for power. The CubeSats would be deployed in a string-of-pearls formation from a P-POD launcher into a low Earth orbit for coordinated science measurements over multiple years. Attitude control would rely on passive gravity
This document discusses non-radioisotope power systems for solar system exploration missions without access to sunlight. It mentions using plutonium-238, lithium, sulfur hexafluoride, aluminum, water, magnesium, and carbon dioxide in potential power systems. It also summarizes the science goals and expected data collection of the ALIVE Venus lander mission, including instruments to measure atmospheric structure, composition, and meteorology and collect descent imagery and panoramic photos.
This document discusses using shepherd satellites to provide guidance, navigation, and control for arrays of microsatellites performing formation flying. It proposes using optical scattering and gradient forces generated by lasers on the shepherd satellites to apply corrective forces to the microsatellite array from a distance. Analytic models predict these radiation forces could provide restorative forces of 10-5 N to 10-4 N using laser powers of 10-10 kW to 100 kW. Potential applications include drag makeup for low Earth orbiting satellites, position control for array formation, and correcting perturbations in geosynchronous Earth orbit.
This document provides a design study for a proposed CubeSat mission called SWaRMM (Space Weather and Radiation Multi-point Magnetometry) that would deploy six 0.5U CubeSats in a slowly separating string to conduct multi-point magnetometer measurements. Each CubeSat would carry a single mini fluxgate magnetometer to characterize phenomena like EMIC waves and Birkeland currents. Preliminary designs for the CubeSats include a structure to carry solar panels and a payload boom, an electrical power system using solar cells and batteries, and attitude control possibly using gravity gradient and hysteresis rods. Initial analyses show the design could meet power and mass requirements to achieve the science goals of the low-cost
Simulation of Deployment and Operation of an Earth Observing SatelliteAlber Douglawi
1) A simulation was conducted of a spacecraft deploying from a launch vehicle and performing attitude control to point its sensor at targets on Earth. Initially, the spacecraft tumbled out of the launch vehicle and thrusters were used to detumble it and align with the local horizontal frame.
2) During operations, a targeting algorithm prioritized 1000 targets and reaction wheels oriented the spacecraft to point at the highest value targets within its sensor range every 100 seconds. Over one day, this allowed it to image 235 targets worth a total of $67461.
3) Disturbance torques from the gravity gradient, solar radiation pressure, aerodynamics, and flexing of deployed solar panels and sensor were modeled. Gains
1) MagBeam is a proposed plasma propulsion system that uses focused plasma beams and magnetic fields to transfer power and thrust separately from spacecraft payloads, enabling fast, efficient propulsion for multiple space missions.
2) Laboratory experiments at the University of Washington have demonstrated the focusing and guiding of plasma beams over short distances using magnetic fields, with the goal of scaling this technology up for applications requiring kilometers of beam propagation.
3) Preliminary analyses suggest MagBeam could enable dramatic mass and cost savings over chemical propulsion for applications like transferring payloads to low Earth orbit, geosynchronous orbit, and missions to Mars through reusable, high-efficiency plasma thrusters.
This document summarizes a presentation about satellite communication. It discusses the basic concept of a communication satellite, how satellites are used as relay stations to transmit signals between Earth stations, and the different types of satellite orbits including geostationary, low Earth, and medium Earth orbits. It also covers topics like inter-satellite links, routing between satellites, common modulation techniques, and recent developments in satellite communication technology.
The document discusses spatial control of photons and optical vortices. It describes how photons can be put into Laguerre-Gaussian modes using mode converters or holograms. These modes carry orbital angular momentum and can be used to encode quantum information. Precise control over generation, manipulation, and measurement of photon states enables applications in quantum communication.
A dwarf galaxy is colliding with the large spiral galaxy NGC 1232, as revealed by X-ray observations from Chandra. The collision is creating a large region (7.25 kpc in diameter) of shocked, hot gas with a temperature of around 5.8 million kelvin. The X-ray luminosity of this collisional aftermath is estimated to be 3.7x10^38 ergs/s. Based on the size and temperature of the X-ray emitting region, the collision likely involves a dwarf galaxy and represents a massive energy input into NGC 1232, far exceeding a typical supernova. Such collisions detected solely in X-rays may provide insights into the role of dwarf galaxy interactions in the evolution of
New Post-DART Collision Period for the Didymos System: Evidence for Anomalous...Sérgio Sacani
On September 26, 2022, NASA’s DART spacecraft impacted Dimorphos, the secondary asteroid in
the (65803) Didymos system, so that the efficiency with which a satellite could divert an asteroid
could be measured from the change in the system’s period. We present new data from the Thacher
Observatory and measure a change in period, ∆P = −34.2 ± 0.1 min, which deviates from previous
measurements by 3.5 σ. This suggests that the system period may have decreased by ∼ 1 minute in
the 20 to 30 days between previous measurements and our measurements. We find that no mechanism
previously presented for this system can account for this large of a period change, and drag from impact
ejecta is an unlikely explanation. Further observations of the (65803) Didymos system are needed to
both confirm our result and to further understand this system post impact.
1. The document contains multiple choice and structured questions about gravitation.
2. Questions cover topics like gravitational field strength at different heights, gravitational forces between celestial bodies, and equations for orbital motion.
3. Sample problems are worked out relating to gravitational forces, escape velocities, and the distribution of molecular speeds as it relates to atmospheric evolution.
Control Systems For Projectile DefenseRyan MendivilMar.docxmaxinesmith73660
Control Systems For Projectile Defense
Ryan Mendivil
March 20, 2015
Abstract
In this paper, I will describe various methods for defending against airborne projectiles. This includes
tracking mechanisms for following objects in three dimensional space and predicting what paths they will
take. In addition, methods of calculating interception trajectories and the factors involved will be discussed.
Contents
I Introduction 1
II Assumptions 2
III Model 2
1 Projectile Tracking 3
1.1 Radar . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
1.2 Camera . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2 Calculating Trajectories 4
2.1 Line and Curve Fitting . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.2 Kalman Filtering . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
3 Intercepting 5
3.1 Aim and Travel Time . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
3.2 Solving For Trajectories . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
4 Verification 7
5 Discussion 7
6 References 8
1
Part I
Introduction
In our modern world, we live in relatively peaceful times. However, there are still may places with ongoing
conflicts. Every year there are around hundreds of soldiers and civilian injured or killed in combat. A good
portion of these casualties come from the use of projectile based weaponry. When used properly, projectiles
can be very accurate and cause minimal collateral damage. Unfortunately, this is not the case in many
modern war zones. Projectiles are launched with the intent to cause harm to anyone from the opposing
side, be they civilians or soldiers. Producing systems that can properly prevent this kind of attack is of
vital importance. There are already many systems on the market but most are extremely expensive and
proprietary. Producing open systems that can be used across a wide range of hardware would be beneficial
to all. This paper will discuss a general model of control that can be applied to projectile tracking and
defense.
Part II
Assumptions
• The projectile is within tracking distance of our system and is distinguishable from it’s surroundings.
• The system will have a clean line of sight to the enemy projectile when it fires.
• A hit will be considered successful when both the enemy projectile and our intercepting projectile
occupy the same space.
• The time it takes the system to aim is constant or is set to large enough to account for any possible
amount of movement.
• The accuracy and sampling rate of the projectile tracker is high enough to provide reasonable data.
• The acceleration of the enemy projectile is constant.
• The velocity of our projectile is consistent and the time it will take to reach the point of interception
is calculable.
• The force of gravity on both.
The document discusses methods for characterizing the global environment using satellite data to help overcome challenges posed by weather effects on missile defense sensors. It describes adjusting infrared imagery thresholds to approximate radar observations, extracting weather event boundaries, projecting 3D shapes onto a model Earth, and using an existing satellite constellation to provide continuous coverage. The goal is to determine visibility and sensor performance to optimize sensor selection and placement for missile defense.
This document summarizes the Regolith & Environment Science, and Oxygen & Lunar Volatile Extraction (RESOLVE) mission architecture for prospecting and utilizing lunar resources. Key aspects include:
The RESOLVE rover payload will conduct a 10-day surface mission at the Cabeus crater near the lunar south pole in May 2016. The payload will acquire samples up to 1m deep and characterize volatiles and perform ISRU demonstrations to extract oxygen.
A solar-powered rover was selected as the architecture to survive a long mission, range far from the landing site, and have the lowest risk. The 243kg rover will survey 3,000m powered by a 250W solar array and 3,
This document provides an overview of remote sensing including:
1. The history of remote sensing from early aerial photography to modern satellite systems.
2. The principles of electromagnetic radiation and how different sensors capture radiation in various parts of the spectrum to analyze objects.
3. The various types of remote sensing platforms, sensors, and resolutions including spatial, spectral, temporal, and radiometric and how they provide information.
4. Common applications of remote sensing like land use mapping, change detection, environmental monitoring, and more.
This document provides an overview of remote sensing including:
1. The history of remote sensing from early aerial photography to modern satellite systems.
2. The principles of electromagnetic radiation and how different sensors capture radiation in various parts of the spectrum to analyze objects.
3. The various types of remote sensing platforms, sensors, and data products including satellites, spectral resolution, spatial resolution, temporal resolution, and applications like land cover mapping.
This document provides an overview of remote sensing including:
1. The history of remote sensing from early aerial photography to modern satellite systems.
2. The principles of electromagnetic radiation and how different sensors capture radiation in various parts of the spectrum to analyze objects.
3. The various types of remote sensing platforms, sensors, and data products including satellites, spectral resolution, spatial resolution, temporal resolution, and applications like land cover mapping.
This project uses computer simulations to model observations of the 2005 Deep Impact collision with comet Tempel 1. The simulations aim to understand the physics behind the light curves observed by Hubble Space Telescope. The simulations suggest the optically thick ejecta cloud was about 28 km in diameter 13 minutes after impact and expanding at around 36 m/s, constraining the cloud's mass to approximately 2x10^7 kg. This mass and expansion velocity are consistent with independent estimates from observations by different astronomy groups.
An almost dark galaxy with the mass of the Small Magellanic CloudSérgio Sacani
This document describes the discovery and characterization of an almost dark galaxy named Nube. Deep imaging with GTC revealed Nube has an extremely low surface brightness of 26.7 mag/arcsec^2 and a stellar mass of 4x10^8 solar masses. Follow-up observations with GBT detected HI emission from Nube, suggesting it is located 107 Mpc away. At this distance, Nube has a large half-mass radius of 6.9 kpc and low effective stellar density, making it the most extended low-surface brightness galaxy found. Its properties are difficult to reproduce in CDM simulations but are consistent with an ultra-light dark matter particle model.
Initial Calibration of CCD Images for the Dark Energy Survey- Deokgeun ParkDaniel Park
The document describes initial calibration of images from the Dark Energy Survey (DES) test run on the Cerro Tololo Inter-American Observatory 1-meter telescope in Chile. Standard star images taken in different atmospheric conditions (airmasses) were used to determine the relationship between measured and true star brightness. This relationship accounts for effects of atmosphere and allows calibration of images to determine true brightness of other stars, important for measuring galaxy redshifts and studying dark energy driving the expansion of the universe, the focus of the full DES study.
This document provides an overview of Vandana Manral's summer training at ONGC regarding satellite communication. It discusses advantages and disadvantages of satellite communication, different orbit types including LEO, MEO, and GEO. It describes components of satellites and earth stations, including modules on satellites and specifications of ONGC's earth station. Frequency bands and multiple access techniques used in satellite communication are also summarized. The training focused on understanding satellite communication systems used by ONGC for its operations.
This document discusses remote sensing platforms and technologies used to create maps from satellite and aerial imagery. It covers different types of satellite orbits used for earth observation, as well as the various sensors and imaging capabilities of satellites. Key points covered include polar versus non-polar orbits, types of remote sensing like passive and active, different spectral and spatial resolutions, and digital data formats for satellite imagery.
This document discusses plate tectonics and earthquakes. It outlines learning objectives about plate boundaries and the distribution of volcanoes, quakes, and mountains. It then discusses determining an earthquake's epicenter using triangulation of arrival times at three seismic stations. An activity is described to locate the epicenter of a hypothetical quake using this method. The importance of determining the epicenter is to help emergency response and preparedness for future quakes.
Here are the answers to the exam questions:
Q1. By using equations for potential and kinetic energy, derive the equation for escape velocity:
Total energy at infinity (Etot) = Kinetic energy (Ek)
1/2mv^2 = GMm/r
For an object to escape, Etot must be positive or zero.
1/2mv^2 = -GMm/r
mv^2 = 2GM/r
v = √(2GM/r)
Q2. Calculate the escape velocity for the following planets:
a) Mars: mass = 6.46 × 1023 kg, radius = 3.39 × 106 m
Escape velocity
This document provides an outline and overview of key concepts in astronomy related to light and telescopes. It discusses:
1. The electromagnetic spectrum and different types of electromagnetic radiation used in astronomy like visible light, infrared, ultraviolet, X-rays, and radio waves.
2. Optical telescopes and their components like lenses, mirrors, and eyepieces. It also covers concepts like light gathering power, resolving power, and magnification.
3. Modern telescope designs that are lighter, computer-controlled, and use techniques like adaptive optics to improve image quality.
4. Other types of telescopes like radio telescopes and how interferometry is used to improve their resolving power by combining signals from
3. the data to the station. The Schriever Air Force base is at, latitude 38.8027 deg and longitude
104.522 deg. The map can be seen in Figure 1 with both targets and receiver facility.
Target Latitude (deg) Longitude (deg)
1 25.7202 97.08
2 25.5 97.23
3 26.23 99.01
4 27.36 99.35
5 29.44 101.25
6 29.46 102.37
7 28.58 103.07
8 29.33 104.39
9 30.36 105.02
10 31.43 106.23
11 31.47 108.12
12 31.19 108.12
13 31.19 111.06
14 32.29 114.48
15 32.43 114.43
16 32.32 117.07
Table 1. Target Locations along Border
Figure 1. Targets and Facility Location
Next the initial orbit has to be made following the requirements set for the project;
inclination +33 deg to 33 deg, and an orbit of 14 to 16 revs/day. The satellite will have a
TwoBody setup in the STK program. This will give us a semiaxis of 6671 km and then the mean
motion will be 15.9337 rev/day, which will be a period of 5422.47 sec. The first orbit can be
seen in Figure 2.
4.
Figure 2. Initial Orbit
Once the initial orbit is chosen the constellation will be built to give max coverage.
Figure 35 show three different constellation setups. The chosen constellation in the end was
the one that had the least gap over a long period of time. Once that was set it was what gave
the best coverage, Constellation 1 was eventually the one chosen.
Figure 3. Constellation 1 Figure 2. Constellation 2
Figure 4. Constellation 3
5.
The details for the 16 satellites in the constellation can be seen in Table 2. This will show
the inclination, argument of perigee, RAAN, and the true anomaly.
Table 2. Satellite Information for Orbit
Figure 5 and 6 will show the constellation coverage over two of the targets. Since the
coverage is very similar for every target, only two graphs will need to be shown, the min and
max time. All the targets have a max time of not being seen of around 12 minutes. Since it is
very difficult for an individual or group to cross the border in that time it is an acceptable
constellation. Table 3 will then show the total coverage for the targets over a 24hr period and
the max non coverage time.
Table 3. Coverage of Every Target
7.
Figure 8. Energy transmission vs. wavelength
The aperture diameter was calculated from:
.34mD = Res
2.44λ(SR)
= 1m
2.44×2.1×10 m×274.55×10 m−6 3
= 1
Then the size of the payload was calculated from the size of a Multispectral MidIR(Table 4).
Aperture Diameter 1m
Linear Dimension(Length) 1.5m
Linear Dimension(Diameter) 1m
Mass 800kg
Power 900W
Table 4.Multispectral MidIR Payload size
So the aperture ratio for the satellite in the project is calculated to be 1.34, and other size
properties can be calculated. The results are shown in Table 5.
Aperture Diameter 1.34m
Linear Dimension(Length) 2.01m
Linear
Dimension(Diameter)
1.34m
Mass 1191.8kg
Power 2165.49W
Table 5. Payload Size for the project(K=1)
Assume a 10% duty cycle, the average power is 216.549W. A scale drawing is in the Appendix.
From DMC project, the pixel diameter was assumed to be 7 μm. The focal length was
calculated :
.10mf = x
hd
= 1m
300×10 m×7×10 m3 −6
= 2
So the magnification is 7E06 and number of pixel was calculated to be:
8. pixel SW 00, 00# = λ
magnification = 1 0
Then the image plane radius and angular field of view are calculated:
m .35mrd = 2
100,000
× 7 × 10−6
= 0
Include a 10% margin, rd=0.385m
°tan 0.662 θ = 2 −1
(f
rd
)= 2
To keep a 0.5kn stability, the angular field of view should be 20.662°±0.211°. The Muiltspectral
MidIR payload has a pointing accuracy of 0.1 deg which satisfies the requirement of 0.211 deg.
Finally, the performance of the payload was decided: Ground speed and data
performance.
390.39m/sV g = P
2πRE
= 7
And based on the ground speed, the sensor should image 7390 swaths per sec. We assume the
data for a pixel is 8 bits. The data for a swath is 800,000 bits. The data per orbit is
00, 00bits/swath 390swath/s 422.47s .206 bits/orbit8 0 × 7 × 5 = 3 × 1013
By assuming the duty cycle to be 10%, the data per orbit is 3.206E12 bits. So the data storage
for one satellite should be 4E11 Bytes which is 373.2GBytes. Assume the average pass time over
the ground station is 15 minutes, the satellite requires a transmitting data rate of 424
MBytes/sec.
Electrical Power Subsystem Design
The EPS Design included the design of the solar plane based on the power consumption
and eclipse time analysis and the battery design.
For the power consumption and eclipse time analysis. The power budget is shown in Table 6
Payload 40% 216.55W
Structure 0 0
Thermal 0 0
Power 10% 54.138W
TT&C 20% 108.275W
ADCS 15% 181.206W
Propulsion 5% 27.069W
Total 100% 541.375W
Table 6. Power Budget
9. From STK simulation, the eclipse time is 2193.06s and daylight time is 3229.41s. Assume the
power loads during eclipse and daylight are the same. The daylight and eclipse efficiency
and which are the same as DMC electrical power subsystem..8Xd = 0 .6Xe = 0
67.95W Psa = Td
+Xd
P Td d
Xe
P Te e
= 7
At the beginning of the life, the power density solar array generated is
Flux)(ξ)(I )cosθ PBOL = ( d
Assume the input solar density is 1367 , efficiency of solar cell is 28% and inherent/mW 2
degradation is 0.77 as DMC used. The satellite used suntracking solar panel so the sunlight
incidence angle is 0. The power density output at the beginning of life is calculated as 294.724
. The satellite required a 10 years life and 1% degradation per year was assumed. The/mW 2
power density output at the end of life was calculated:
(1 %) 66.54W/mPEOL = PBOL − 1 10
= 2 2
So the area of solar panel is 2.881 .m2
Then for the battery design, NiH battery was used. In 10 years life, the battery need to charge
and discharge for and0years 65.25days 4hours 600sec/5422.37sec 8198cycles1 × 3 × 2 × 3 = 5
from Figure 9, the depth of discharge should be 35%.
Figure 9. Depth of discharge vs. cycle life
Assume one battery is used and the transmission efficiency between battery and load n is 0.9
which is a typical used value, the battery capacity should be:
10. 046.973W r Cr = P Te e
(DOD)Nn = 1 ∙ h
Use the same kind of battery as DMC, the energy density is 50 Whr/kg. The battery mass is
20.939kg.
Communication
Communications satellites allow telephone and data conversations to be relayed
through the satellite.The most important feature of a communications satellite is the
transponder a radio that receives a conversation at one frequency and then amplifies it and
retransmits it back to Earth on another frequency. A satellite normally contains hundreds or
thousands of transponders.
Communication satellites are all in geosynchronous orbit, meaning that they stay in one place
in the sky relative to the Earth. “The signal transmitted between the spacecraft and the ground
station, or between two spacecraft, must arrive at the receiver with enough strength to be
detected. The strength of the received signal depends upon: Strength of the signal transmitted
(power density in the desired direction) Amount of attenuation due to the medium
(atmospheric attenuation, path loss, etc) Sensitivity of the receiver (ability to focus received
signal and detect information)”.
Each satellite is launched into space at about 300 km above the Earth. At this speed and
altitude, the satellite will revolve around the planet approximately 15 times every 24 hours.
Constraints that had been set for the communication design approved to operate at RF
frequencies 2.2 GHz downlink and 2.5 GHz uplink, ground Station (GS) receiver gain 3.0,
receiver bandwidth 200 KHz, and a receiver temperature: 20°C.
Uplink is the frequency at which ground control is communicating with the satellite and
downlink is when the satellite transponder convert the signal and send it down to the second
earth station.
14. structure 85.5 6937.16542 1935.1654651
thermal 15.6 750.41657 353.1654
Electrical power 135 11679.60983 4863.36463
TT&C 15 1823.465673 515.3465459
TT&C 15 1823.465673 515.3465459
C&DH
ADCS 22.3 5740.3208 3643.32457
Propulsion 32.6 262.46543 144.62321
Grand Total 27033.456
To calculate the unit cost, we used the equation as follows:
And the unit costs of all the parts of the satellite are calculated as: (with the conversion into
FY00$)
Unit number Production cost Unit cost (FY00$K)
1 27033.456 27033.456
2 51567.1564 25359.37655
3 69534.67448 23546.67234
4 82467.6461 20925.0431
5 116732.9431 20345.7793
6 136476.9235 20245.71601
7 159985.4315 23576.6725
8 163449.983 19573.37697
15. 9 189822.354 19437.35595
10 203978.359 19234.4622
11 229460.357 16542.802
12 242591.7496 19345.432
13 256347.3243 18231.32465
14 282364.3457 19254.2545
15 301972.3784 18348.4256
16 315753.3541 18346.95234
Total Cost 323.7 Million
Therefore, the total cost would be the total operation cost(Launch vehicle cost) plus the Cost of
16 satellites, which is 353.7M+ 175M= 498.7M
So our design is right under the budget, which met the constraint and requirement of the
mission.
17.
Redundancies Rsystem [1 1 A) n] 1 1 B) n] .. n − 1 = − ( − R ˆ * [ − ( − R ˆ * .
System Reliabilities with various redundancies of systems:
# of
Redundancies
Rsystem
(10 yr)
P(16/16)
(%)
16/R
P(16/{16/R})
(%)
Nadj
P(16/Nadj)
(%)
0 .0892 1.6*10^15 180 N/A N/A N/A
1 .5136 2.3*10^3 32 62.98 41 95.91
2 .7977 2.69 21 76.08 24 96.13
3 .9189 25.84 18 82.48 20 98.06
4 .9672 59.14 17 89.43 18 98.01
5 .9866 80.59 17 97.86 17 97.86
As you increase the number of redundancies, the system noticeably becomes more reliable.
Then I adjust the number of satellites to be the minimum number needed to have a probability
of 95% or higher that at least 16 satellites will survive the mission. This results in our ideal case
of 4 redundancies and 18 satellites.
19. Aerodynamic Drag Torque:
v = [μe/R]^.5 = 7.73 km/s
Ta max = .5*Roatm*Cd*SA *(Cp Cg)*v^2
=1.000*10^5 N m
Solar Pressure Torque:
As ≈ (15 m)*(3 m) = 45 m^2
Tsrp = Fs*As*(1 + q)*(1)*(Cp Cg)/c
=.990*10^4 N m
System will accommodate Total Disturbance Torque:
Td = ∑(Tx^2)^.5
= 5.460*10^4 N m
Conclusion
The design met all the requirements and the budget for 16 satellites is just under $500M. The
longest break of the coverage is 12 minutes which is believed to be an accepted value.
However, the budget is not sufficient for 18 satellites which is the ideal case for a high
reliability. The potential solution is to use another existing payload characteristics for scaling to
decrease the payload of the project satellite. Decreasing the payload to under 800kg will allow to
launch 18 satellites under the budget requirements.
Appendix
Scale drawing of the satellite