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Air enters a turbojet engine at \(320 \mathrm{m} / \mathrm{s}\) at a rate of \(30 \mathrm{kg} / \mathrm{s},\) and exits at \(650 \mathrm{m} / \mathrm{s}\) relative to the aircraft. The thrust developed by the engine is \((a) 5 \mathrm{kN}\) \((b) 10 \mathrm{kN}\) \((c) 15 \mathrm{kN}\) \((d) 20 \mathrm{kN}\) \((e) 26 \mathrm{kN}\)

Short Answer

Expert verified
(a) 5 kN (b) 10 kN (c) 15 kN (d) 20 kN Answer: (b) 10 kN

Step by step solution

01

Identify the given parameters and the thrust formula

We are given: - Air entering velocity (Vi) = 320 m/s - Air exiting velocity (Ve) = 650 m/s (relative to the aircraft) - Mass flow rate (m) = 30 kg/s We'll use the thrust formula: Thrust (T) = m * (Ve - Vi)
02

Calculate the change in velocity

We need to find the difference between the exiting and entering velocities. So, subtract the entering velocity from the exiting velocity: ΔV = Ve - Vi = 650 m/s - 320 m/s = 330 m/s
03

Calculate the thrust

Now, use the thrust formula and the values we found for mass flow rate (m) and change in velocity (ΔV): T = m * ΔV = 30 kg/s * 330 m/s = 9900 N
04

Convert thrust to kN and find the answer

Now, we need to convert the thrust from Newtons (N) to kilonewtons (kN) by dividing by 1000: Thrust (T) = 9900 N / 1000 = 9.9 kN ≈ 10 kN The thrust developed by the turbojet engine is approximately 10 kN. Therefore, the correct answer is (b) 10 kN.

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Key Concepts

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

Thrust Formula
Understanding how to calculate the thrust generated by a turbojet engine is critical for students diving into the world of aerospace engineering. Thrust is the forward force that propels the aircraft through the air and is a result of Newton's third law of motion — for every action, there is an equal and opposite reaction.

In the simplest terms, the thrust formula can be expressed as:

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Most popular questions from this chapter

A gas-turbine power plant operates on the simple Brayton cycle between the pressure limits of 100 and 800 kPa. Air enters the compressor at \(30^{\circ} \mathrm{C}\) and leaves at \(330^{\circ} \mathrm{C}\) at a mass flow rate of \(200 \mathrm{kg} / \mathrm{s}\). The maximum cycle temperature is \(1400 \mathrm{K}\). During operation of the cycle, the net power output is measured experimentally to be 60 MW. Assume constant properties for air at \(300 \mathrm{K}\) with \(c_{\mathrm{v}}=0.718 \mathrm{kJ} / \mathrm{kg} \cdot \mathrm{K}, c_{p}=\) \(1.005 \mathrm{kJ} / \mathrm{kg} \cdot \mathrm{K}, R=0.287 \mathrm{kJ} / \mathrm{kg} \cdot \mathrm{K}, k=1.4\) (a) Sketch the \(T\) -s diagram for the cycle. (b) Determine the isentropic efficiency of the turbine for these operating conditions. (c) Determine the cycle thermal efficiency.

How do the inefficiencies of the turbine and the compressor affect \((a)\) the back work ratio and \((b)\) the thermal efficiency of a gas-turbine engine?

Consider an ideal gas-turbine cycle with one stage of compression and two stages of expansion and regeneration. The pressure ratio across each turbine stage is the same. The highpressure turbine exhaust gas enters the regenerator and then enters the low-pressure turbine for expansion to the compressor inlet pressure. Determine the thermal efficiency of this cycle as a function of the compressor pressure ratio and the high-pressure turbine to compressor inlet temperature ratio. Compare your result with the efficiency of the standard regenerative cycle.

An Otto cycle with air as the working fluid has a compression ratio of \(10.4 .\) Under cold-air-standard conditions, the thermal efficiency of this cycle is \((a) 10\) percent (b) 39 percent \((c) 61\) percent \((d) 79\) percent \((e) 82\) percent

Why are the back work ratios relatively high in gasturbine engines?

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