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Helium gas is flowing through a duct. At a particular location it is at \(150 \mathrm{kPa}\) and \(300 \mathrm{~K}\), and it has a velocity of \(280 \mathrm{~m} / \mathrm{s}\). Assume that Helium behaves as an ideal gas. Determine (a) the Mach number. (b) the stagnation temperature in \(\mathrm{K}\). (c) the stagnation pressure in kPa.

Short Answer

Expert verified
(a) 0.278 (b) 302.3 K (c) 152.4 kPa

Step by step solution

01

Title - Calculate the Speed of Sound

The speed of sound in an ideal gas can be found using the formula: \[ a = \sqrt{\gamma R T} \]where \(\gamma\) is the specific heat ratio for Helium (which is 1.66), \(R\) is the specific gas constant for Helium (2077 J/kg·K), and \(T\) is the temperature in Kelvin (300 K). Substituting the values, we get: \[ a = \sqrt{1.66 \times 2077 \times 300} \approx 1006.4 \ \text{m/s} \]
02

Title - Calculate the Mach Number

The Mach number is given by: \[ M = \frac{v}{a} \]where \(v\) is the local velocity of the flow (280 m/s). Substituting the values, we get: \[ M = \frac{280}{1006.4} \approx 0.278 \]
03

Title - Calculate the Stagnation Temperature

The stagnation temperature is given by: \[ T_0 = T \left(1 + \frac{\gamma - 1}{2} M^2 \right) \]where \(T\) is the temperature (300 K), \(\gamma\) is the specific heat ratio (1.66), and \(M\) is the Mach number (0.278). Substituting the values, we get: \[ T_0 = 300 \left(1 + \frac{1.66 - 1}{2} \times 0.278^2 \right) \approx 302.3 \ \text{K} \]
04

Title - Calculate the Stagnation Pressure

The stagnation pressure is given by: \[ P_0 = P \left(1 + \frac{\gamma - 1}{2} M^2 \right)^{\frac{\gamma}{\gamma - 1}} \]where \(P\) is the pressure (150 kPa), \(\gamma\) is the specific heat ratio (1.66), and \(M\) is the Mach number (0.278). Substituting the values, we get: \[ P_0 = 150 \left(1 + \frac{1.66 - 1}{2} \times 0.278^2 \right)^{\frac{1.66}{1.66 - 1}} \approx 152.4 \ \text{kPa} \]

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Key Concepts

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

Mach number calculation
To find the Mach number, we first need to calculate the speed of sound in Helium at a given temperature. This is important because Mach number is defined as the ratio of the flow velocity to the speed of sound. The speed of sound in an ideal gas can be found using the formula: \[ a = \sqrt{\gamma R T } \]Where:
  • \( \gamma \) is the specific heat ratio, which for Helium is 1.66,
  • \( R \) is the specific gas constant for Helium, equal to 2077 J/kg·K.
  • \( T \) is the temperature in Kelvin, given as 300 K.
Substituting the values into the formula gives us:\[ a = \sqrt{1.66 \times 2077 \times 300} \approx 1006.4 \text{m/s} \]Next, we use the calculated speed of sound to find the Mach number with the velocity of the flow:\[ M = \frac{v}{a} \]Where:
    z
  • \( v \) is the local velocity of the flow, which is 280 m/s.
Substituting the values, we get:\[ M = \frac{280}{1006.4} \approx 0.278 \]This tells us that the flow velocity is approximately 27.8% of the speed of sound.
stagnation temperature
The stagnation temperature is the temperature of the gas when it is brought to rest adiabatically. It accounts for the kinetic energy of the flowing gas.The formula to calculate the stagnation temperature is:\[ T_0 = T \(1 + \frac{\gamma - 1}{2} M^2 \) \]Where:
  • \( T \) is the static temperature, which is 300 K.
  • \( \gamma \) is the specific heat ratio, which is 1.66.
  • \( M \) is the Mach number, which we have calculated as 0.278.
Substituting the values, we get:\[ T_0 = 300 \(1 + \frac{1.66 - 1}{2} \times 0.278^2 \) \approx 302.3 \text{K} \]This means that if the gas was brought to rest isentropically, its temperature would increase slightly to 302.3 K.
stagnation pressure
Stagnation pressure is the pressure a fluid attains when it is brought to rest isentropically. It represents the maximum possible pressure of the gas.The formula to calculate the stagnation pressure is:\[ P_0 = P \(1 + \frac{\gamma - 1}{2} M^2 \)^{\frac{\gamma}{\gamma - 1}} \]Where:
  • \( P \) is the static pressure, given as 150 kPa.
  • \( \gamma \) is the specific heat ratio, which is 1.66.
  • \( M \) is the Mach number, which we calculated as 0.278.
Substituting the values, we get:\[ P_0 = 150 \(1 + \frac{1.66 - 1}{2} \times 0.278^2 \)^{\frac{1.66}{1.66 - 1}} \approx 152.4 \text{kPa} \]This indicates that the pressure would increase slightly to 152.4 kPa if the flow were brought to rest isentropically.
ideal gas law
The ideal gas law is a fundamental equation that describes the relationship between the pressure, volume, temperature, and amount of gas. Although it is not explicitly needed for the specific calculations in the exercise, it provides a fundamental understanding of gas behavior.The ideal gas law is given by the equation:\[ PV = nRT \]Where:
  • \( P \) is the pressure of the gas.
  • \( V \) is the volume of the gas.
  • \( n \) is the number of moles of the gas.
  • \( R \) is the universal gas constant, 8.314 J/mol·K.
  • \( T \) is the temperature of the gas in Kelvin.
Rearranging for specific gas constants and moles for practical use, it can also be written as:\[ P = \rho RT \]Where \( \rho \) is the density of the gas. This form makes it easier to apply directly when dealing with fluid dynamics, such as calculating parameters in a flowing gas, where density, pressure, and temperature are often the variables of interest.

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Most popular questions from this chapter

Consider a modification of the air-standard Otto cycle in which the isentropic compression and expansion processes are each replaced with polytropic processes having \(n=1.25\). The compression ratio is 10 for the modified cycle. At the beginning of compression, \(p_{1}=1\) bar and \(T_{1}=298 \mathrm{~K}\) and \(V_{1}=2200 \mathrm{~cm}^{3}\). The maximum temperature during the cycle is \(1900 \mathrm{~K}\). Determine (a) the heat transfer and work in \(\mathrm{kJ}\), for each process in the modified cycle. (b) the thermal efficiency. (c) the mean effective pressure, in bar.

Liquid water at \(25^{\circ} \mathrm{C}\) flows at steady state through a \(7 \mathrm{~cm}\)-diameter horizontal pipe. The mass flow rate is \(15 \mathrm{~kg} / \mathrm{s}\). The pressure decreases by \(12 \mathrm{kPa}\) from inlet to exit of the pipe. Determine the magnitude, in \(\mathrm{N}\), and direction of the horizontal force required to hold the pipe in place.

An engine working on the air standard Otto cycle is supplied with air at \(0.1 \mathrm{MPa}, 27^{\circ} \mathrm{C}\). The compression ratio is 8 . The heat supplied is \(1400 \mathrm{~kJ} / \mathrm{kg}\). Calculate the maximum pressure and temperature of the cycle, the cycle efficiency, and the mean effective pressure.

The ideal Brayton and Rankine cycles are composed of the same four processes, yet look different when represented on a \(T-s\) diagram. Explain.

A simple gas turbine is the topping cycle for a simple vapor power cycle (Fig. 9.23). Air enters the compressor of the gas turbine at \(15^{\circ} \mathrm{C}, 100 \mathrm{kPa}\), with a volumetric flow rate of \(20 \mathrm{~m}^{3} / \mathrm{s}\). The compressor pressure ratio is 12 and the turbine inlet temperature is \(1440 \mathrm{~K}\). The compressor and turbine each have isentropic efficiencies of \(88 \%\). The air leaves the interconnecting heat exchanger at \(460 \mathrm{~K}, 100 \mathrm{kPa}\). Steam enters the turbine of the vapor cycle at \(7000 \mathrm{kPa}, 480^{\circ} \mathrm{C}\), and expands to the condenser pressure of \(7 \mathrm{kPa}\). Water enters the pump as saturated liquid at \(7 \mathrm{kPa}\). The turbine and pump efficiencies are 90 and \(70 \%\), respectively. Cooling water passing through the condenser experiences a temperature rise from 15 to \(27^{\circ} \mathrm{C}\) with a negligible change in pressure. Determine (a) the mass flow rates of the air, steam, and cooling water, each in \(\mathrm{kg} / \mathrm{s}\). (b) the net power developed by the gas turbine cycle and the vapor cycle, respectively, each in \(\mathrm{kJ} / \mathrm{s}\). (c) the thermal efficiency of the combined cycle. (d) a full accounting of the net exergy increase of the air passing through the combustor of the gas turbine, \(\dot{m}_{\text {air }}\left[\mathrm{e}_{t 3}-\mathrm{e}_{42}\right]\), in \(\mathrm{kJ} / \mathrm{s}\). Discuss. Let \(T_{0}=300 \mathrm{~K}, p_{0}=100 \mathrm{kPa}\).

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