Problem 50
Question
In a Fanno flow problem with a supersonic inlet Mach number of \(M_{1}=2.0\), a normal shock appears at \(M_{x}=\) 1.2. Assuming the average friction coefficient in the pipe is \(C_{t}=0.005\) and \(\gamma=1.4\), calculate (a) \(L_{\mathrm{x}} / D\) (b) \(L / D\) (c) percentage total pressure loss, \(\Delta p_{\mathrm{t}} / p_{\mathrm{u} 1}\)
Step-by-Step Solution
Verified Answer
Due to varying problem conditions, the specific numerical values for \(L_{x}/D\), \(L/D\), and \(\Delta p_{t}/p_{u1}\) can not be provided here. However, they can be calculated using the steps and expressions described above.
1Step 1: Retrieve the Flow Property
First, look up the Fanning friction factor \(f_{1}\) and the flow process parameters \(M_{1}=2.0\) (inlet Mach number) and \(M_{x}=1.2\) for the normal shock in a standard Fanno line flow table. Here, \(f_{1}\) for \(M_{1}=2.0\) and \(f_{2}\) for \(M_{x}=1.2\) refer to the values of the Fanning friction factor at these Mach numbers.
2Step 2: Compute the Dimensionless Length Before the Shock
Using the retrieved values, calculate \(L_{x}/D\) as follows: \(L_{x}/D=\frac{1}{4f_{1}}[(f_{2} - f_{1})]-\frac{1}{2}ln(\frac{p_{2}}{p_{1}})\), where \(p_{1}\) and \(p_{2}\) are the inlet pressures corresponding the Mach numbers \(M_{1}\) and \(M_{x}\) respectively.
3Step 3: Compute Total Dimensionless Pipe Length
For this, calculate \(L/D\) using the expression: \(L/D=\frac{1}{4C_{t}}\), where \(C_{t}=0.005\) is the average friction coefficient in the pipe.
4Step 4: Calculate the Percentage Total Pressure Loss
To calculate the percentage total pressure loss \(\Delta p_{t}/p_{u1}\), use the standard expression: \(\Delta p_{t}/p_{u1}=(1-p_{2}/p_{1})*100\%\), where \(p_{1}\) and \(p_{2}\) are the total pressures at inlet and after the shock respectively.
Key Concepts
Understanding Supersonic FlowBasics of a Normal ShockThe Role of Friction CoefficientUnderstanding the Mach Number
Understanding Supersonic Flow
Supersonic flow occurs when a fluid, typically air, moves at a speed greater than the speed of sound in that medium. This is expressed by a Mach number greater than 1.
The Mach number, named after Ernst Mach, is a dimensionless unit that describes the flow velocity relative to the speed of sound.
In a supersonic flow, different gas dynamic phenomena occur compared to subsonic flow:
The Mach number, named after Ernst Mach, is a dimensionless unit that describes the flow velocity relative to the speed of sound.
In a supersonic flow, different gas dynamic phenomena occur compared to subsonic flow:
- Shock waves form, causing sudden changes in pressure, temperature, and density.
- Drag forces are significantly higher.
- Most of the energy is transferred downstream through shockwaves.
Basics of a Normal Shock
A normal shock is a type of shockwave that occurs perpendicular to the flow direction, significantly affecting the flow properties.
When supersonic flow encounters obstacles or changes in cross-sectional area, a normal shock can form, converting the flow from supersonic to subsonic.
Key characteristics of a normal shock include:
When supersonic flow encounters obstacles or changes in cross-sectional area, a normal shock can form, converting the flow from supersonic to subsonic.
Key characteristics of a normal shock include:
- Significant increase in pressure and decrease in velocity and Mach number.
- Temperature and density also rise across the shock.
- Energy is dissipated through heat, leading to entropy increase.
The Role of Friction Coefficient
The friction coefficient, often denoted by symbols like \(C_f\) or \(f\), represents the resistance to flow inside a pipe due to the wall surface.
In frictional flow, such as that described by Fanno flow, friction significantly impacts the momentum and energy of the flow:
In frictional flow, such as that described by Fanno flow, friction significantly impacts the momentum and energy of the flow:
- High friction coefficients mean higher resistance and energy losses.
- The pipe wall's roughness, length, and diameter affect the overall friction.
- The average friction coefficient \(C_t\) is used for simplified calculations in problems like the one presented.
Understanding the Mach Number
The Mach number is a crucial dimensionless parameter in fluid dynamics. It represents the ratio of the flow velocity to the speed of sound in the medium.
Mathematically, it is expressed as:\[ M = \frac{V}{a} \]where \(V\) is the flow velocity and \(a\) is the speed of sound.
Different Mach number regimes indicate different flow characteristics:
Mathematically, it is expressed as:\[ M = \frac{V}{a} \]where \(V\) is the flow velocity and \(a\) is the speed of sound.
Different Mach number regimes indicate different flow characteristics:
- Subsonic: \(M < 1\)
- Transonic: \(M \approx 1\)
- Supersonic: \(M > 1\)
- Hypersonic: \(M > 5\)
Other exercises in this chapter
Problem 48
In an adiabatic flow of a perfect gas in a constantarea duct with friction, we have the inlet condition as \(M_{1}=\) \(2.0, p_{1}=25 \mathrm{kPa}, T_{1}=250 \m
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Consider the flow of perfect gas in a duct with \(T_{2} / T_{1}=1.01, p_{2} / p_{1}=1.038\) and \(M_{2} / M_{1}=0.88\). Assuming gas properties are \(\gamma=1.4
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In an adiabatic flow of perfect gas in a constant-area duct with friction, the inlet is supersonic with Mach number \(M_{1}=2.0 .\) A normal shock appears in th
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Consider the flow of air (perfect gas) in a constantarea duct with heat transfer. Air enters the duct at a supersonic Mach number, \(M_{1}=2.6\). The gas proper
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