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Assume that the flowrate, \(Q\) of a gas from a smokestack is a function of the density of the ambient air, \(\rho_{a},\) the density of the gas, \(\rho_{g},\) within the stack, the acceleration of gravity, \(g\) and the height and diameter of the stack, \(h\) and \(d\), respectively. Use \(\rho_{a}, d,\) and \(g\) as repeating variables to develop a set of pi terms that could be used to describe this problem.

Short Answer

Expert verified
The three dimensionless \(\pi\) terms are \(\pi_1 = \frac{Q}{\rho_a d^{5/2} g^{1/2}}\), \(\pi_2 = \frac{\rho_g}{\rho_a}\), and \(\pi_3 = \frac{h}{d}\).

Step by step solution

01

Identify the Variables

List all the relevant variables for the problem. We have the flowrate \(Q\) of the gas, ambient air density \(\rho_{a}\), gas density \(\rho_{g}\), the acceleration due to gravity \(g\), and the stack dimensions \(h\) and \(d\).
02

Choose Repeating Variables

Choose repeating variables which appear in most of the dimensional groups and whose combination covers all the fundamental dimensions involved. Here, we choose \(\rho_{a}\), \(d\), and \(g\) as the repeating variables, as the problem instructs.
03

Apply Buckingham Pi Theorem

According to Buckingham Pi Theorem, the dimensional analysis will produce \(n - k\) independent \(\pi\) terms, where \(n\) is the number of variables, and \(k\) is the number of repeating variables. We have 6 variables (\(Q, \rho_{a}, \rho_{g}, g, h, d\)) and 3 repeating variables, thus 6 - 3 = 3 \(\pi\) terms.
04

Form the Pi Terms

Form each \(\pi\) term by combining the repeating variables and the remaining variables. For each \(\pi\) term, ensure the overall group is dimensionless. Solve for exponents to balance the dimensions.- \(\pi_1: Q = [\rho_{a}^a d^b g^c]\)- \(\pi_2: \rho_{g} = [\rho_{a}^a d^b g^c]\)- \(\pi_3: h = [\rho_{a}^a d^b g^c]\)
05

Solve for Each Pi Term

Set up and solve equations for the coefficients for each \(\pi\) term by equating dimensions on both sides:- For \(\pi_1: [L^3/T] = [M^a L^b (L/T^2)^c]\), solve for \(a, b, c\).- For \(\pi_2: [M/L^3] = [M^a L^b (L/T^2)^c]\), solve for \(a, b, c\).- For \(\pi_3: [L] = [M^a L^b (L/T^2)^c]\), solve for \(a, b, c\).
06

Express Pi Terms Dimensionlessly

After calculating coefficients, write \(\pi\) terms:- \(\pi_1 = \frac{Q}{\rho_a d^{5/2} g^{1/2}}\)- \(\pi_2 = \frac{\rho_g}{\rho_a}\)- \(\pi_3 = \frac{h}{d}\)

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Key Concepts

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

Buckingham Pi Theorem
The Buckingham Pi Theorem is a fundamental principle in dimensional analysis that helps simplify complex physical systems by reducing the number of variables involved. When dealing with problems like calculating the flowrate of gas from a smokestack, this theorem becomes particularly useful. It allows us to express a problem in terms of dimensionless parameters, called pi terms, which encapsulate all the pertinent dimensional characteristics.

How does it work? The theorem states that if you have an equation with \(n\) dimensional variables, and \(k\) of them are independent repeating variables, you can simplify this system into \(n - k\) dimensionless products (pi terms). Each pi term results from the combination of repeating variables with one non-repeating variable to achieve a dimensionless parameter. The key advantage is that these pi terms apply universally, irrespective of the specific units being used.

This principle not only helps in simplifying calculations but also enhances the understanding of the underlying physics, by allowing researchers to study the effects of scale and other input variable changes without necessarily running numerous experiments. In our exercise, we use this theorem to determine three dimensionless pi terms by combining six variables: \(Q, \rho_a, \rho_g, g, h,\) and \(d\), three of which are chosen as repeating.
Repeating Variables
Repeating variables are a key concept in simplifying problems using the Buckingham Pi Theorem. These variables appear in many or all of the dimensionless pi terms in a given problem. To choose the right repeating variables, they must meet specific criteria.

Choosing repeating variables involves:
  • They must cover all fundamental dimensions such as mass \(M\), length \(L\), and time \(T\).
  • They should appear in most of the dimensional groups.
  • Avoid choosing variables that are themselves dimensionless.
In the smokestack flowrate problem, \(\rho_a, d,\) and \(g\) are selected as repeating variables because:
  • They cover dimensions of density, length, and acceleration.
  • They help form dimensionless terms when paired with other non-repeating variables \(Q, \rho_g,\) and \(h\).
Repeating variables play a crucial role because they ensure that each resulting pi term is dimensionally balanced, leading to the formation of coherent dimensionless parameters.
Flowrate in Fluid Dynamics
Flowrate, in the context of fluid dynamics, refers to the volume of fluid passing through a cross-section per unit time. It's an essential parameter in analyzing fluid systems like smokestacks, pipelines, or rivers. In our exercise, the flowrate \(Q\) is influenced by several physical properties such as the densities of ambient air \(\rho_a\) and gas \(\rho_g\), gravity \(g\), and the smokestack's dimensions \(h\) and \(d\).

Flowrate calculations often involve:
  • Density: Different densities between ambient air and gas influence buoyancy and thus flowrates.
  • Gravity: Influences the potential flow energy and velocity of the gas.
  • Stack Dimensions: Height \(h\) and diameter \(d\) affect how quickly and efficiently the gas flows upward.
Understanding flowrate is vital for designing and optimizing systems to ensure they operate safely and efficiently. By utilizing tools like dimensional analysis, engineers can predict how different factors affect the flowrate, enabling better design choices and operational strategies.

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Most popular questions from this chapter

A cone and plate viscometer consists of a cone with a very small angle \(\alpha\) that rotates above a flat surface as shown in Fig. P7.21. The torque, \(\mathscr{T}\), required to rotate the cone at an angular velocity \(\omega\) is a function of the radius, \(R,\) the cone angle, \(\alpha,\) and the fluid viscosity, \(\mu,\) in addition to \(\omega .\) With the aid of dimensional analysis, determine how the torque will change if both the viscosity and angular velocity are doubled.

Flow patterns that develop as winds blow past a vehicle, such as a train, are often studied in low-speed environmental (meteorological wind tunnels. (See Video \(\mathrm{V} 7.16 .\) ) Typically, the air velocities in these tunnels are in the range of \(0.1 \mathrm{m} / \mathrm{s}\) to \(30 \mathrm{m} / \mathrm{s}\). Consider a cross wind blowing past a train locomotive. Assume that the local wind velocity, \(V,\) is a function of the approaching wind velocity (at some distance from the locomotive), \(U,\) the locomotive length, \(\ell\) height, \(h,\) and width, \(b,\) the air density, \(\rho,\) and the air viscosity, \(\mu\). (a) Establish the similarity requirements and prediction equation for a model to be used in the wind tunnel to study the air velocity, \(V\) around the locomotive. (b) If the model is to be used for cross winds gusting to \(U=25 \mathrm{m} / \mathrm{s}\), explain why it is not practical to maintain Reynolds number similarity for a typical length scale 1: 50 .

Assume that the drag, \(\mathscr{P}\), on an aircraft flying at supersonic speeds is a function of its velocity, \(V\), fluid density, \(\rho\), speed of sound, \(c,\) and a series of lengths, \(\ell_{1}, \ldots, \ell_{i},\) which describe the geometry of the aircraft. Develop a set of pi terms that could be used to investigate experimentally how the drag is affected by the various factors listed. Form the pi terms by inspection.

The flowrate, \(Q,\) of water in an open channel is assumed to be a function of the cross-sectional area of the channel, \(A\), the height of the roughness of the channel surface, \(\varepsilon,\) the acceleration of gravity, \(g,\) and the slope, \(S_{0},\) of the hill on which the channel sits. Put this relationship into dimensionless form.

It is desired to determine the wave height when wind blows across a lake. The wave height, \(H,\) is assumed to be a function of the wind speed, \(V\), the water density, \(\rho\), the air density, \(\rho_{a}\), the water depth, \(d\), the distance from the shore, \(\ell\), and the acceleration of gravity, \(g\), as shown in Fig. P7.7. Use \(d, V\), and \(\rho\) as repeating variables to determine a suitable set of pi terms that could be used to describe this problem.

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