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What is the difference between the upstream velocity and the free-stream velocity? For what types of flow are these two velocities equal to each other?

Short Answer

Expert verified
Answer: Upstream and free-stream velocities are equal in situations where the flow is uniform and not affected by any boundaries or obstacles, such as idealized, uniform (or parallel) flows where fluid velocities remain constant and don't vary in the direction perpendicular to the main flow direction. Examples include inviscid flows (with no viscosity) or unidirectional flows in a wind tunnel.

Step by step solution

01

Define the upstream velocity

Upstream velocity refers to the velocity at a point in the flow that is not directly impacted by the presence of an obstacle, such as a solid boundary or object.
02

Define the free-stream velocity

Free-stream velocity is the velocity of the fluid in the undisturbed flow, far away from any boundaries or obstacles in the fluid.
03

Differentiate between upstream velocity and free-stream velocity

The difference between upstream velocity and free-stream velocity lies in their relation to obstacles or boundaries present within the flow: - The upstream velocity is measured at a specific point in the fluid that is not directly affected by the presence of an obstacle or boundary but is still within the flow. - The free-stream velocity is a reference velocity that represents the undisturbed fluid velocity far away from any boundaries or obstacles.
04

Determine the conditions in which upstream and free-stream velocities are equal

In a flow without any boundaries or obstacles, the fluid velocities would be uniform and both the upstream and free-stream velocities would be equal. This can occur in an idealized, uniform (or parallel) flow, where the flow doesn't vary in the direction perpendicular to the main flow direction. Examples include inviscid flow (no viscosity) or unidirectional flow in a wind tunnel.

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Key Concepts

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

Fluid Mechanics
Fluid mechanics is a branch within physics that deals with the properties and behavior of fluids—in both liquid and gas phases—and the forces acting upon them. It provides the framework for analyzing fluid flow, whether the fluid is stationary or in motion. Understanding the principles of fluid mechanics is essential for analyzing various phenomena such as flow through pipes, aerodynamics of an aircraft, blood circulation in the body, and even weather patterns.

In fluid mechanics, the study of flows includes various aspects such as velocity, pressure, density, and temperature as functions of space and time. This study can be categorized into hydrodynamics for liquid flow and aerodynamics for gas flow. Moreover, the principles of fluid mechanics are applied in different flow regimes which include laminar and turbulent flows, each with its own set of complexities.
Flow Velocity Concepts
The flow velocity of a fluid is a vector quantity that represents the direction and magnitude of the fluid's motion at a point in space. It is a fundamental concept in fluid mechanics as it largely determines the resultant force that a fluid may exert on an object within it. Flow velocity can vary from point to point and is influenced by factors such as the fluid's properties, the shape and size of passages through which the fluid travels, and the presence of obstacles or boundaries.

It is important to differentiate between different types of velocities when studying fluid flow:
  • Local velocity: The velocity at a specific point within a fluid.
  • Average velocity: The average speed of fluid across a certain cross-sectional area.
  • Uniform velocity: When the velocity does not change from point to point in the fluid.
Note that in most real-world scenarios, the velocity of fluids varies throughout the flow field, and this variation has profound effects on the overall behavior of the fluid.
Boundary Layer Theory
Boundary layer theory is a fundamental part of fluid mechanics that describes the behavior of fluid flow near a surface (boundary). When a real fluid with viscosity flows past a solid surface, the fluid particles directly in contact with the surface adhere to it due to the no-slip condition. As one moves away from the surface, the velocity of the fluid increases until it reaches what is known as the free-stream velocity.

This velocity gradient from zero at the boundary to the free-stream velocity at some distance away forms the boundary layer. The thickness of this layer is determined by the viscosity of the fluid and the shape of the surface. Within this layer, the effects of viscosity are significant and dominate the flow characteristics, leading to a reduction in flow velocity near the surface. The study of boundary layers is essential in engineering applications involving aerodynamics and hydrodynamics because it affects drag forces and heat transfer rates.
Inviscid Flow
Inviscid flow refers to the idealized flow condition where the fluid's viscosity is assumed to be zero. In such cases, internal friction within the fluid is neglected, simplifying the analysis of the fluid's behavior. This assumption is used in many theoretical fluid dynamics problems because it allows for a focus on the effects of pressure and velocity without the complicating factors of viscous shear stress.

In reality, there is no such thing as a perfectly inviscid fluid; however, the concept is useful for approximating the behavior of fluids when the influence of viscosity is very small compared to other forces. For example, high-speed flows such as those encountered in aerodynamics at large scales can often be treated as inviscid. In these scenarios, the upstream velocity, which is the velocity approaching an object, and the free-stream velocity far from the object can be approximately considered equal, meaning the effects of viscosity and boundaries on the flow are negligible.

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Most popular questions from this chapter

Warm air is blown over the inner surface of an automobile windshield to defrost ice accumulated on the outer surface of the windshield. Consider an automobile windshield \(\left(k_{w}=\right.\) \(0.8 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot \mathrm{R})\) with an overall height of 20 in and thickness of \(0.2\) in. The outside air ( \(1 \mathrm{~atm})\) ambient temperature is \(8^{\circ} \mathrm{F}\) and the average airflow velocity over the outer windshield surface is \(50 \mathrm{mph}\), while the ambient temperature inside the automobile is \(77^{\circ} \mathrm{F}\). Determine the value of the convection heat transfer coefficient for the warm air blowing over the inner surface of the windshield, necessary to cause the accumulated ice to begin melting. Assume the windshield surface can be treated as a flat plate surface.

Air at \(20^{\circ} \mathrm{C}\) flows over a 4-m-long and 3-m-wide surface of a plate whose temperature is \(80^{\circ} \mathrm{C}\) with a velocity of \(5 \mathrm{~m} / \mathrm{s}\). The rate of heat transfer from the surface is (a) \(7383 \mathrm{~W}\) (b) \(8985 \mathrm{~W}\) (c) \(11,231 \mathrm{~W}\) (d) 14,672 W (e) \(20,402 \mathrm{~W}\) (For air, use \(k=0.02735 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=0.7228, \nu=1.798 \times\) \(\left.10^{-5} \mathrm{~m}^{2} / \mathrm{s}\right)\)

Jakob (1949) suggests the following correlation be used for square tubes in a liquid cross-flow situation: $$ \mathrm{Nu}=0.102 \mathrm{Re}^{0.625} \operatorname{Pr}^{1 / 3} $$ Water \((k=0.61 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=6)\) flows across a \(1-\mathrm{cm}\) square tube with a Reynolds number of 10,000 . The convection heat transfer coefficient is (a) \(5.7 \mathrm{~kW} / \mathrm{m}^{2} \cdot \mathrm{K}\) (b) \(8.3 \mathrm{~kW} / \mathrm{m}^{2} \cdot \mathrm{K}\) (c) \(11.2 \mathrm{~kW} / \mathrm{m}^{2} \cdot \mathrm{K}\) (d) \(15.6 \mathrm{~kW} / \mathrm{m}^{2} \cdot \mathrm{K}\) (e) \(18.1 \mathrm{~kW} / \mathrm{m}^{2} \cdot \mathrm{K}\)

A \(20 \mathrm{~mm} \times 20 \mathrm{~mm}\) silicon chip is mounted such that the edges are flush in a substrate. The substrate provides an unheated starting length of \(20 \mathrm{~mm}\) that acts as turbulator. Airflow at \(25^{\circ} \mathrm{C}(1 \mathrm{~atm})\) with a velocity of \(25 \mathrm{~m} / \mathrm{s}\) is used to cool the upper surface of the chip. If the maximum surface temperature of the chip cannot exceed \(75^{\circ} \mathrm{C}\), determine the maximum allowable power dissipation on the chip surface.

How are the average friction and heat transfer coefficients determined in flow over a flat plate?

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