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13.37 Octane gas \(\left(\mathrm{C}_{8} \mathrm{H}_{18}\right)\) at \(25^{\circ} \mathrm{C}\) enters a jet engine and burns completely with \(300 \%\) of theoretical air entering at \(25^{\circ} \mathrm{C}\), 1 atm with a volumetric flow rate of \(42 \mathrm{~m}^{3} / \mathrm{s}\). Products of combustion exit at \(990 \mathrm{~K}, 1 \mathrm{~atm}\). If the fuel and air enter with negligible velocities, determine the thrust produced by the engine in \(\mathrm{kN}\).

Short Answer

Expert verified
Calculate the air-fuel ratio, mass flow rates, and exhaust velocity to find the thrust.

Step by step solution

01

Determine the stoichiometric air-fuel ratio

For the complete combustion of octane \(\text{C}_{8} \text{H}_{18}\), the balanced chemical equation is: \[ \text{C}_{8} \text{H}_{18} + 12.5\text{O}_2 + 3.76(12.5\text{N}_2) \rightarrow 8\text{CO}_2 + 9\text{H}_2O + 3.76(12.5\text{N}_2) \] The stoichiometric air-fuel ratio by mass is given by the formula: \[ \frac{\text{mass of air}}{\text{mass of fuel}} = \frac{12.5(32 + 3.76 \times 28.97)}{114} \] Calculate this ratio.
02

Calculate theoretical and actual air flow rates

Given that actual air is 300% of theoretical, we can write: \[ \text{Actual air flow} = 3 \times \text{Theoretical air flow} \] The volumetric flow rate of air at standard conditions (25^{\text{C}}, 1 ATM) is provided as 42 m^3/s. Use the ideal gas law to convert this to mass flow rate: \[ \text{mass flow rate of air, } \text{ṁ}_{\text{air}} = \frac{\text{volumetric flow rate} \times \text{density}}{ \text{molar mass} } \]where density at standard conditions can be found using \[ \text{density} = \frac{\text{P}}{\text{R} \times \text{T}} \]
03

Find mass flow rate of octane

Determine the mass flow rate of fuel using the air to fuel ratio from Step 1 and the mass flow rate of air from Step 2: \[ \text{ṁ}_{\text{fuel}} = \frac{\text{ṁ}_{\text{air}}}{\text{A/F ratio}} \]
04

Calculate the velocity of expelled gases

Using the mass of products and the ideal gas law, find the velocity of exhaust gases exiting at 990 K and 1 ATM. The exhaust velocity, \[ V_e = \frac{\text{volumetric flow rate}}{\text{cross-sectional area}} \] Determine the volumetric flow rate of the exhaust gases by considering the complete combustion process.
05

Calculate thrust produced

Using the momentum equation for thrust calculation: \[ F = \text{ṁ}_{\text{fuel}} \times V_e \] Simplify this with the values obtained from previous steps to determine the thrust force.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

stoichiometric air-fuel ratio
The stoichiometric air-fuel ratio is critical in ensuring complete combustion of a fuel. In our case, we are working with octane (\text{C}_8 \text{H}_{18}). The balanced chemical equation for the complete combustion is: \[ \text{C}_8 \text{H}_{18} + 12.5\text{O}_2 + 3.76(12.5\text{N}_2) \rightarrow 8\text{CO}_2 + 9\text{H}_2O + 3.76(12.5\text{N}_2) \] Here, we need to calculate the mass air-fuel ratio. This ratio is calculated using the formula: \[ \frac{\text{mass of air}}{\text{mass of fuel}} = \frac{12.5(32 + 3.76 \times 28.97)}{114} \] This ratio helps us know how much air is needed to fully burn 1 kg of fuel under ideal conditions. If we have too much fuel or too little air, combustion will be incomplete, wasting fuel and producing more pollution.
mass flow rate
The mass flow rate, \text{ṁ}, refers to the amount of mass traveling through a cross-section per unit time. It’s typically measured in kilograms per second (kg/s). For our jet engine problem, we have the following steps to calculate the mass flow rates:
  • We start with the volumetric flow rate of air which is given as 42 m^3/s at standard conditions.
  • Using the ideal gas law, we convert this volumetric flow rate to mass flow rate.
The mass flow rate of air can be determined using the equation: \[ \text{ṁ}_{\text{air}} = \frac{\text{volumetric flow rate} \times \text{density}}{ \text{molar mass} } \] Density at standard conditions can be calculated using: \[ \text{density} = \frac{\text{P}}{\text{R} \times \text{T}} \]
ideal gas law
The ideal gas law is a fundamental equation in thermodynamics, describing the behavior of ideal gases. It is written as: \[ \text{PV} = \text{nRT} \] where P is pressure, V is volume, n is number of moles, R is the ideal gas constant (8.314 J·mol^-1·K^-1), and T is temperature. In our problem, the ideal gas law helps us convert the volumetric flow rate of the air into a mass flow rate. Using rearrangement, we get: \[ \text{n} = \frac{\text{P} \times \text{V}}{\text{R} \times \text{T}} \] By evaluating n, the number of moles, we can then find the mass using the molar mass relation: \[ \text{mass} = \text{n} \times \text{molar mass} \]
combustion process
Combustion is a chemical process where fuel reacts with an oxidant, releasing heat and producing products like CO2, H2O, etc. For our octane (C8H18) in the jet engine, combustion can be defined by the balanced equation: \[ \text{C}_8 \text{H}_{18} + 12.5\text{O}_2 + 3.76(12.5\text{N}_2) \rightarrow 8\text{CO}_2 + 9\text{H}_2O + 3.76(12.5\text{N}_2) \] To ensure complete combustion, sufficient oxygen is essential. We use a stoichiometric ratio to determine the precise amounts of fuel and air needed for complete combustion. This process converts chemical energy in the fuel into thermal energy, which in turn, gets used for propulsion by the jet engine.
momentum equation
Thrust in a jet engine is a result of the momentum change of gases. The thrust can be determined using the momentum equation: \[ F = \text{ṁ}_{\text{fuel}} \times V_e \] Where F is the thrust, \text{ṁ}_{\text{fuel}} is the mass flow rate of the fuel, and V_e is the exhaust velocity. In our problem, we calculate the velocity of the expelled gases at the nozzle exit. Given that we know the mass flow rates and exhaust conditions, we can determine thrust effectively. This equation essentially measures how fast the exhaust gases are pushed out of the engine, propelling the jet forward.

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Most popular questions from this chapter

13.1D The term acid rain is frequently used today. Define what is meant by the term. Discuss the origin and consequences of acid rain. Also discuss options for its control.

13.43 For a natural gas with a molar analysis of \(86.5 \% \mathrm{CH}_{4}, 8 \%\) \(\mathrm{C}_{2} \mathrm{H}_{6}, 2 \% \mathrm{C}_{3} \mathrm{H}_{8}, 3.5 \% \mathrm{~N}_{2}\), determine the lower heating value, in \(\mathrm{kJ}\) per \(\mathrm{kmol}\) of fuel and in \(\mathrm{kJ}\) per \(\mathrm{kg}\) of fuel, at \(25^{\circ} \mathrm{C}, 1 \mathrm{~atm}\).

13.35 The energy required to vaporize the working fluid passing through the boiler of a simple vapor power plant is provided by the complete combustion of methane with \(110 \%\) of theoretical air. The fuel and air enter in separate streams at \(25^{\circ} \mathrm{C}, 1 \mathrm{~atm}\). Products of combustion exit the stack at \(150^{\circ} \mathrm{C}\), \(1 \mathrm{~atm}\). Plot the mass flow rate of fuel required, in \(\mathrm{kg} / \mathrm{h}\) per MW of power developed by the plant versus the plant thermal efficiency, \(\eta\). Consider \(\eta\) in the range \(30-40 \%\). Kinetic and potential energy effects are negligible.

13.60 Streams of hydrogen \(\left(\mathrm{H}_{2}\right)\) and oxygen \(\left(\mathrm{O}_{2}\right)\), each at \(1 \mathrm{~atm}\), enter a fuel cell operating at steady state and water vapor exits at \(1 \mathrm{~atm}\). If the cell operates isothermally at (a) \(300 \mathrm{~K}\), (b) \(400 \mathrm{~K}\), and (c) \(500 \mathrm{~K}\), determine the maximum theoretical work that can be developed by the cell in each case, in kJ per kmol of hydrogen flowing, and comment. Heat transfer with the surroundings takes place at the cell temperature, and kinetic and potential energy effects can be ignored.

13.9 A coal sample has a mass analysis of \(80.4 \%\) carbon, \(3.9 \%\) hydrogen \(\left(\mathrm{H}_{2}\right), 5.0 \%\) oxygen \(\left(\mathrm{O}_{2}\right), 1.1 \%\) nitrogen \(\left(\mathrm{N}_{2}\right), 1.1 \%\) sulfur, and the rest is noncombustible ash. For complete combustion with \(120 \%\) of the theoretical amount of air, determine the air-fuel ratio on a mass basis.

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