/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 53 A compressor stage at its pitchl... [FREE SOLUTION] | 91Ó°ÊÓ

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A compressor stage at its pitchline radius \(\left(r_{\mathrm{m}}=0.25\right)\) has \({ }^{\circ} R_{\mathrm{m}}=0.73\). The axial velocity is constant at \(C_{2 m}=150\) \(\mathrm{m} / \mathrm{s}\). The flow entering the compressor is swirl free, i.e., \(\alpha_{1}=0\). The flow exiting the stage at pitchline is also swirl free, i.e., \(\alpha_{3}=0 .\) The compressor angular speed is \(\omega=7500 \mathrm{rpm}\). The speed of sound at the entrance to the stage is \(a_{1}=330 \mathrm{~m} / \mathrm{s}\) and rotor solidity at the pitchline radius is \(\sigma_{\mathrm{m}}=0.80\). Assuming the gas constant is \(R=287 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\) and \(\gamma=1.4\), calculate: (a) absolute swirl downstream of the rotor, \(C_{\theta 2 \mathrm{~m}}\), in \(\mathrm{m} / \mathrm{s}\) (b) rotor specific work at pitchline radius, \(w_{c}\), in \(\mathrm{kJ} / \mathrm{kg}\) (c) total temperature downstream of the rotor, \(T_{12 m}\), in K (d) de Haller criterion for the rotor at pitchline (e) the rotor diffusion factor at the pitchline radius, \(D_{\mathrm{m}}\)

Short Answer

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Step by step solution

01

Calculate Absolute Swirl Downstream of the Rotor

The absolute swirl downstream of the rotor is given by \(C_{\theta2m}=C_{2m}\times R_m\), where \(C_{2m}\) is the axial velocity and \(R_m\) is the reaction ratio. Substitute the given values to obtain the answer.
02

Calculate Rotor Specific Work at Pitchline Radius

The rotor specific work at pitchline radius is given by \(w_c = C_{\theta2m}^2 / 2\), where \(C_{\theta2m}\) is the absolute swirl downstream of the rotor. Use the value of \(C_{\theta2m}\) calculated in Step 1 to find \(w_c\). Remember to convert joules to kilojoules.
03

Calculate Total Temperature Downstream of the Rotor

The total temperature downstream of the rotor is given by \(T_{12m} = T_{11m} + w_c / cp\), where \(cp\) is the specific heat capacity at constant pressure. Given that \(cp = R (\gamma / (\gamma - 1))\), substitute the values to find \(cp\). \(T_{11m}\) is the total temperature upstream of the rotor and is equal to the temperature at entrance to the stage, which is \(a_1^2 / (2cp)\). Substitute all the found values to find \(T_{12m}\).
04

Calculate De Haller Criterion

De Haller criterion is given by \(C_{2m} / C_{1m}\). Given that the flow is swirl free at inlet, \(C_{1m} = C_{1a}\) which is the absolute entry velocity. We know that \(C_{1a} = \sqrt{(2cp*T_{11m})}\). Substitute these values to find De Haller criterion.
05

Calculate Rotor Diffusion Factor

The rotor diffusion factor at pitchline is given by \(D_m = 1 - (C_{2m} / C_{1m})^2\). Use the found values for \(C_{2m}\) and \(C_{1m}\) to calculate \(D_m\).

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Key Concepts

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

Compressor Stage Analysis
Understanding compressor stage analysis is essential in the field of aerodynamics and aircraft engineering. By analyzing a stage in an aircraft compressor, engineers can determine the performance and efficiency of the compressor. A typical stage includes a set of rotating blades known as the rotor followed by a set of stationary blades called the stator. The pitchline radius, mentioned in the exercise, is a specific radial location within the compressor where measurements are often taken for simplicity and because it is representative of the overall performance.

In analyzing compressor stages, one of the key performance metrics is the absolute swirl, or the circumferential component of the velocity downstream of the rotor—which in this case is influenced by the axial velocity and the reaction ratio. The specific work done by the rotor on the air reflects the energy addition to the working fluid and is proportional to the square of the absolute swirl. These metrics are critical to optimizing stage performance and ensuring the compressor delivers the necessary pressure rise to the air moving through the engine.

Engineers also calculate the increase in total temperature across the rotor, utilizing thermodynamic relationships. The De Haller criterion is an indicator of the stability of the flow within the compressor. It compares the axial velocity at the inlet and outlet of a stage. Low values can indicate potential flow separation and poor stage performance. Similarly, the rotor diffusion factor is a measure of the decrease in velocity across the rotor, providing insights into the diffusion process which if excessive, can lead to flow separation and efficiency loss.
Axial Compressor Aerodynamics
Axial compressors are a crucial component within turbo machinery, found in jet engines and industrial gas turbines. They compress air by accelerating it with a set of rotors and diffusing it through stators, which results in a pressure increase. The exercise discusses the aerodynamics at play in such a compressor. The values like the axial velocity and the swirl-free condition at the entrance and exit of the compressor's stage are parameters describing how the fluid moves within the compressor.

The aerodynamic performance of an axial compressor is largely determined by the behavior of the flow within the bladed passages. Controlling the flow to ensure it remains attached to the blades is critical for efficient operation. Factors such as solidity, which is the blade chord length divided by the spacing between the blades at a specific radial position, play a role in determining the compressor's ability to effectively compress the fluid without stalling or surging.

In practice, designers aim to achieve a balance between the axial and swirling components of the flow to maximize energy transformation while minimizing losses due to shock waves, turbulence, and boundary layer effects. Understanding axial compressor aerodynamics helps in designing more efficient stages that can operate stably over a wide range of conditions.
Thermodynamics in Propulsion
The principles of thermodynamics are fundamental in understanding propulsion systems, like those found in aircraft engines. These principles help in predicting the behavior of gases under various temperatures and pressures, which is crucial for designing components like compressors and turbines. In our exercise, thermodynamics is applied to determine the total temperature downstream of the rotor, which signifies the energy level of the gas after work has been done on it by the rotor blades.

The compressor works by converting kinetic energy into pressure energy, and the relationship between the temperature, work, and heat transfer is described by the first law of thermodynamics. The specific work input to the air can be seen as an increase in the total (or stagnation) temperature of the gas. The gas constant and the heat capacity ratio (denoted by the symbol \(\gamma\)) are thermodynamic properties of air, and they are crucial in calculating the specific heat capacities which determine how much energy is needed to raise the temperature of the working fluid.

Understanding these thermodynamic relationships is essential for engineers to design propulsion systems that are not only efficient but also reliable and capable of providing the necessary thrust for flight. The concepts of specific work, heat capacity, and total temperature play a direct role in the performance of an aircraft's propulsion system, dictating how effectively the engine can convert fuel into kinetic energy.

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Most popular questions from this chapter

A compressor stage has 37 rotor blades and 41 stator blades. The shaft rotational speed is \(5000 \mathrm{rpm}\). Calculate (a) the rotor blade passing frequency as seen by the stator blades (b) the stator blade passing frequency as seen by the rotor blades

In an axial-flow compressor test rig with no inlet guide vanes, a 1 -m diameter fan rotor blade spins with a sonic tip speed, i.e., \(U_{\text {tip }} / a_{1}=1.0 .\) If the speed of sound in the laboratory is \(a_{0}=300 \mathrm{~m} / \mathrm{s}\), and the axial velocity to the fan is \(C_{z 1}=150 \mathrm{~m} / \mathrm{s}\), calculate the fan rotational speed \(\omega\) in rpm. $$ R=287 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K} \text { and } \gamma=1.4 $$

The absolute flow to a compressor rotor has a coswirl with \(\alpha_{1}=15^{\circ}\). The exit flow from the rotor has an absolute flow angle \(\alpha_{2}=35^{\circ}\). The pitchline radius is at \(r_{\mathrm{m}}=0.6 \mathrm{~m}\) and the rotor angular speed is \(\omega=5220 \mathrm{rpm}\). Assuming the axial velocity is \(C_{z \mathrm{~m}}=150 \mathrm{~m} / \mathrm{s}\) and is constant across the rotor, calculate (a) the specific work at the pitchline (b) the rotor torque per unit mass flow rate (c) the degree of reaction

A rotor blade row has a hub-to-tip radius ratio of \(0.5\), solidity at the pitchline of \(1.0\), the axial velocity is \(160 \mathrm{~m} / \mathrm{s}\), and zero preswirl. The mean section has a design diffusion factor of \(D_{\mathrm{m}}=0.5\). Calculate and plot where appropriate (a) exit swirl at the pitchline assuming the shaft rpm of 6000 and \(r_{\mathrm{m}}=1.0 \mathrm{ft}(0.3 \mathrm{~m})\) (b) downstream swirl distribution \(C_{\theta 2}\) (r) assuming a freevortex design rotor (c) the radial distribution of degree of reaction \({ }^{\circ} R\) along the blade span (d) radial distribution of diffusion factor \(D_{\mathrm{r}}(r)\).

A compressor stage at the pitchline, \(r_{\mathrm{m}}=0.5 \mathrm{~m}\), is shown. The inlet flow to the rotor has a preswirl with \(\alpha_{1}=\) \(22^{\circ} .\) The axial velocity is \(C_{21}=C_{22}=C_{23}=170 \mathrm{~m} / \mathrm{s}\), i.e. constant throughout the stage. The stage is of repeated design, with \(\alpha_{3}=\alpha_{1} .\) Rotor and stator solidities at pitchline are 1.2 and \(1.0\) respectively. The rotor inlet relative velocity at pitchline is sonic, i.e., \(W_{1}=a_{1}\) and the rotor relative exit velocity, following de Haller criterion, is \(W_{2}=0.75 W_{1}\). Calculate: (a) shaft rotational speed, \(\omega\), in rpm (b) rotor exit (absolute) swirl, \(C_{\theta 2}\) in \(\mathrm{m} / \mathrm{s}\) (c) stage degree of reaction, \({ }^{\circ} R_{\mathrm{w}}\) (d) rotor D-factor, \(D_{\mathrm{r}}\) (e) stage total temperature ratio (f) stage total pressure ratio for \(e_{c}=0.9\)

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