Problem 44
Question
Air enters a constant-area scramjet combustor at Mach 3.2. Assuming the flow is frictionless and the combustion is simulated as external heating of air, use Rayleigh flow to calculate \(q^{*}\) and the fuel-air ratio that is needed to thermally choke the scramjet combustor. The fuel heating value is assumed to be \(118,500 \mathrm{~kJ} / \mathrm{kg}\) of fuel.
Step-by-Step Solution
Verified Answer
After substituting the values and performing the required calculations, we will get the values of \( q^{*} \) and fuel-air ratio \( f \). These values are the solution to the problem.
1Step 1: Find \(q^{*}\)
The Rayleigh flow relation for the critical heat addition in terms of Mach number (using air as working fluid) is given by: \(q^{*}=Cp*T0*(M^{2}-1)\)Where:- \( Cp \) is specific heat at constant pressure, which for air is about 1004.5 J/(kg*K),- \( T0 \) is total temperature. Standard sea level condition (SSL) can be assumed, giving \( T0 = 288.2 K \).- \( M \) is the incoming Mach number, which is given as 3.2.Calculate \( q^{*} \) by substituting these values into the equation.
2Step 2: Calculate Fuel-Air Ratio
The fuel-air ratio \( f \) is given by the equation:\( f = \frac{q^{*}}{h}\)Where:- \( h \) is the specific heat of combustion or heating value of the fuel (given here as 118,500 kJ/Kg or 118,500,000 J/Kg),- \( q^{*} \) is the critical heat addition calculated in Step 1.Substitute the values of \( q^{*} \) and \( h \) into the equation to find the fuel-air ratio \( f \) which is necessary to choke the scramjet combustor.
Key Concepts
Scramjet CombustorMach NumberFuel-Air RatioThermal Choking
Scramjet Combustor
A scramjet combustor is an integral component of a scramjet engine, utilized in high-speed aviation. The term "scramjet" stands for "supersonic combustion ramjet." Unlike traditional jet engines, scramjets operate efficiently at hypersonic speeds (Mach 5 and above). In this system, air enters the combustor at supersonic speeds, and combustion occurs without slowing the flow to subsonic speeds.
This ability to manage supersonic airflow through the combustor allows scramjets to maintain efficiency at extremely high speeds. They lack moving parts, unlike turbojets, which means they are lighter and potentially more robust. However, they require precision in airflow management and ignition timing.
This ability to manage supersonic airflow through the combustor allows scramjets to maintain efficiency at extremely high speeds. They lack moving parts, unlike turbojets, which means they are lighter and potentially more robust. However, they require precision in airflow management and ignition timing.
- Entry airspeed: Supersonic, typically above Mach 3
- Efficiency relies on maintaining supersonic conditions
- No need for complex rotating machinery
Mach Number
The Mach number is a dimensionless quantity representing the ratio of an object's speed to the speed of sound in the surrounding medium. In our context, Mach 3.2 implies the scramjet is flying at 3.2 times the speed of sound. The Mach number is crucial in aerodynamics as it dictates airflow characteristics around a vehicle.
At Mach numbers greater than 1, the flow is supersonic, leading to distinct changes in pressure, temperature, and density across the flow.
At Mach numbers greater than 1, the flow is supersonic, leading to distinct changes in pressure, temperature, and density across the flow.
- Mach 1: Speed of sound (~343 m/s at sea level)
- Greater than Mach 1: Supersonic (e.g., Mach 3.2 means 3.2 times the speed of sound)
- Mach numbers affect shock waves and aerodynamic forces
Fuel-Air Ratio
The fuel-air ratio (\( f \)) is a vital parameter in combustion processes, indicating the proportion of fuel to the mass of air in a combustion chamber. It needs careful calculation to ensure efficient combustion and to prevent overheating or fuel wastage. For scramjets, precise control over this ratio is critical due to the high speeds involved.
The formula used is:\[ f = \frac{q^{*}}{h}\]Where \( q^{*} \) is the heat addition per unit mass of air and \( h \) is the fuel's heating value. Ensuring the correct fuel-air ratio helps achieve optimal combustion efficiency while avoiding thermal choking.
The formula used is:\[ f = \frac{q^{*}}{h}\]Where \( q^{*} \) is the heat addition per unit mass of air and \( h \) is the fuel's heating value. Ensuring the correct fuel-air ratio helps achieve optimal combustion efficiency while avoiding thermal choking.
- Determines efficient fuel combustion
- Key to avoiding overheating or fuel wastage
- Calculated using heat addition and fuel heating value
Thermal Choking
Thermal choking is a condition where increased temperature due to heat addition causes a reduction in flow speed to sonic conditions, effectively choking the flow. In scramjet engines, it is crucial to manage thermal choking to avoid performance degradation.
As heat is added to the supersonic air in the combustor, the density and pressure change, potentially leading to a situation where the flow becomes choked, disrupting the supersonic condition that is vital for scramjet operation.
As heat is added to the supersonic air in the combustor, the density and pressure change, potentially leading to a situation where the flow becomes choked, disrupting the supersonic condition that is vital for scramjet operation.
- Caused by excessive heat addition
- Leads to reduced flow speed
- Critical to avoid in scramjet combustors
Other exercises in this chapter
Problem 42
A scramjet combustor is modeled as a frictionless flow of a perfect gas in a constant-area duct with heating (Rayleigh flow). The inlet Mach number to the burne
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A duct with square cross-section is shown. The inlet flow conditions are known to be: \(M_{1}=0.3, p_{1}=150 \mathrm{kPa}\), \(T_{1}=300 \mathrm{~K}, \gamma=1.4
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Consider an insulated constant-area duct. The average wall friction coefficient is \(C_{1}=0.005\). Assuming the length-to-(hydraulic) diameter ratio for the du
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An inviscid perfect gas flows through a constant-area duct that is subject to heat transfer. The ratio of heat transfer to mass flow rate is \(q=250 \mathrm{~kJ
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