Intro to Aerospace Engineering

šŸ‘©šŸ¼ā€šŸš€Intro to Aerospace Engineering Unit 7 ā€“ Aerospace Propulsion: Jets and Rockets

Aerospace propulsion systems, including jets and rockets, are the driving force behind flight and space exploration. These systems generate thrust by expelling mass, utilizing principles like Newton's third law and the thrust equation to propel vehicles through air and space. Jets and rockets differ in their fuel sources and operational environments. Jet engines use atmospheric air, while rockets carry their own oxidizer, allowing them to function in space. Both types employ various designs and components to optimize performance, efficiency, and specific applications in aviation and spaceflight.

Key Concepts and Terminology

  • Propulsion generates force to move an object, typically by expelling mass in the opposite direction of motion
  • Thrust is the force produced by a propulsion system, measured in newtons (N) or pounds-force (lbf)
  • Specific impulse (IspI_{sp}) measures the efficiency of a propulsion system, expressed as the thrust per unit of propellant flow rate
    • Higher IspI_{sp} indicates better fuel efficiency and performance
  • Propellants are substances used to generate thrust, consisting of fuel and oxidizer
    • Liquid propellants (kerosene, liquid hydrogen) are commonly used in rockets and some jet engines
    • Solid propellants (ammonium perchlorate, aluminum) are used in solid rocket motors
  • Nozzles are essential components that accelerate and direct the exhaust flow to generate thrust
    • Converging-diverging nozzles (De Laval nozzles) are used to achieve supersonic exhaust velocities

Fundamentals of Propulsion

  • Newton's third law of motion states that for every action, there is an equal and opposite reaction, which is the basis for propulsion
  • Propulsion systems generate thrust by expelling mass in the opposite direction of the desired motion
  • Thrust equation: F=mĖ™ve+(peāˆ’p0)AeF = \dot{m}v_e + (p_e - p_0)A_e, where FF is thrust, mĖ™\dot{m} is mass flow rate, vev_e is exhaust velocity, pep_e and p0p_0 are exit and ambient pressures, and AeA_e is nozzle exit area
  • Specific impulse (IspI_{sp}) is a key performance metric for propulsion systems, defined as Isp=FmĖ™g0I_{sp} = \frac{F}{\dot{m}g_0}, where g0g_0 is standard gravity (9.81 m/sĀ²)
    • IspI_{sp} is often expressed in seconds, representing the duration a propulsion system can generate 1 unit of thrust per unit of propellant mass
  • Propulsive efficiency (Ī·p\eta_p) is the ratio of the useful propulsive power to the total power input, given by Ī·p=FvāˆžmĖ™(h0āˆ’he)\eta_p = \frac{F v_{\infty}}{\dot{m} (h_0 - h_e)}, where vāˆžv_{\infty} is the vehicle velocity, and h0h_0 and heh_e are the total enthalpy at the inlet and exit, respectively

Jet Engine Types and Components

  • Jet engines use air as the working fluid and generate thrust by accelerating the air through the engine
  • Turbojet engines compress air using a compressor, burn fuel in a combustion chamber, and expand the hot gases through a turbine and nozzle
    • Suitable for high-speed applications (fighter aircraft) but have lower efficiency at lower speeds
  • Turbofan engines add a large fan before the compressor, which accelerates a larger mass of air around the engine core
    • Bypass ratio is the ratio of the mass flow through the fan to the mass flow through the core
    • High-bypass turbofans (airliners) are more fuel-efficient at subsonic speeds, while low-bypass turbofans (military aircraft) offer better performance at supersonic speeds
  • Turboprop engines use a turbine to drive a propeller, which accelerates a large mass of air to generate thrust
    • Efficient at lower speeds and altitudes (regional and cargo aircraft)
  • Ramjet engines have no moving parts and rely on the forward motion of the vehicle to compress the incoming air
    • Operate efficiently at high supersonic speeds (Mach 3-6) but cannot generate static thrust

Rocket Propulsion Basics

  • Rockets carry both fuel and oxidizer onboard, allowing them to operate in the vacuum of space
  • Chemical rockets burn fuel and oxidizer in a combustion chamber to generate high-temperature, high-pressure gases that are expanded through a nozzle to produce thrust
  • Rocket thrust equation: F=mĖ™ve+(peāˆ’p0)AeF = \dot{m}v_e + (p_e - p_0)A_e, where the second term (pressure thrust) becomes significant at high altitudes or in vacuum
  • Specific impulse for rockets is higher than jet engines due to the absence of air drag and the ability to use more energetic propellants
    • Typical IspI_{sp} values range from 200-300 seconds for solid rockets and 300-450 seconds for liquid rockets
  • Staging is used to improve rocket performance by discarding empty propellant tanks and engines during flight
    • Multistage rockets (Saturn V, Falcon 9) can achieve higher payload mass ratios and reach higher velocities than single-stage rockets

Propellants and Fuel Systems

  • Liquid propellants are stored in separate tanks and pumped into the combustion chamber
    • Bipropellant systems use separate fuel (kerosene, liquid hydrogen) and oxidizer (liquid oxygen) tanks
    • Monopropellant systems use a single propellant that decomposes when heated (hydrazine)
  • Solid propellants are pre-mixed and cast into a solid grain that burns from one end to the other
    • Consist of an oxidizer (ammonium perchlorate), fuel (aluminum), and binder (HTPB)
    • Simpler and more reliable than liquid propellant systems but offer less control over thrust
  • Cryogenic propellants (liquid hydrogen, liquid oxygen) offer high specific impulse but require insulated tanks and careful handling
  • Propellant feed systems can be pressure-fed or pump-fed
    • Pressure-fed systems use pressurized gas to force propellants into the combustion chamber, suitable for small engines
    • Pump-fed systems use turbopumps to deliver propellants at high pressure, necessary for large engines (Space Shuttle Main Engine)

Thrust and Performance Calculations

  • Thrust is calculated using the rocket thrust equation: F=mĖ™ve+(peāˆ’p0)AeF = \dot{m}v_e + (p_e - p_0)A_e
    • Mass flow rate (mĖ™\dot{m}) depends on propellant density, combustion chamber pressure, and nozzle throat area
    • Exhaust velocity (vev_e) is a function of the specific heat ratio, combustion temperature, and pressure ratio across the nozzle
  • Specific impulse is calculated as Isp=FmĖ™g0I_{sp} = \frac{F}{\dot{m}g_0} and represents the efficiency of a rocket engine
    • Affected by factors such as propellant combination, combustion chamber pressure, and nozzle expansion ratio
  • Tsiolkovsky rocket equation describes the relationship between velocity change (Ī”v\Delta v), specific impulse, and initial and final mass: Ī”v=Ispg0lnā”m0mf\Delta v = I_{sp} g_0 \ln \frac{m_0}{m_f}
    • Determines the payload capacity and range of a rocket based on the available propellant mass
  • Thrust-to-weight ratio (TWR) is the ratio of the rocket's thrust to its weight and determines its acceleration and ability to overcome gravity
    • TWR > 1 is necessary for a rocket to lift off from the launch pad

Design Considerations and Challenges

  • Rocket engines must withstand extreme temperatures, pressures, and vibrations during operation
    • Regenerative cooling circulates cryogenic propellant around the nozzle and combustion chamber to prevent overheating
    • Ablative cooling uses a sacrificial material (silica phenolic) that chars and erodes to dissipate heat
  • Throttling and thrust vectoring are used to control the rocket's trajectory and attitude
    • Throttling adjusts the thrust level by varying the propellant flow rate or combustion chamber pressure
    • Thrust vectoring deflects the exhaust flow using movable nozzles or injection of secondary fluids
  • Combustion instability can occur due to pressure oscillations in the combustion chamber, leading to increased heat transfer and structural damage
    • Acoustic cavities, baffles, and injector design are used to dampen instabilities
  • Propellant sloshing in the tanks can affect the rocket's stability and control
    • Baffles and anti-slosh diaphragms are used to minimize sloshing effects
  • Rockets are used for space launch vehicles (SpaceX Falcon, ULA Atlas), spacecraft propulsion (satellites, deep space probes), and military applications (intercontinental ballistic missiles)
  • Electric propulsion systems (ion engines, Hall thrusters) use electricity to accelerate propellant, offering high specific impulse but low thrust
    • Suitable for long-duration missions (Dawn spacecraft) and satellite station-keeping
  • Nuclear thermal rockets heat a propellant (hydrogen) using a nuclear reactor, providing higher specific impulse than chemical rockets
    • Potential for faster interplanetary travel and manned missions to Mars
  • Scramjet (supersonic combustion ramjet) engines enable air-breathing propulsion at hypersonic speeds (Mach 5+)
    • Challenges include efficient fuel injection, mixing, and combustion in supersonic flow
  • Reusable rocket technology (SpaceX Falcon 9, Blue Origin New Shepard) aims to reduce launch costs by recovering and refurbishing rocket stages
    • Vertical takeoff and landing (VTVL) and parachute recovery are the main approaches being developed


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Ā© 2024 Fiveable Inc. All rights reserved.
APĀ® and SATĀ® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.