Chapter 6: Problem 17
The velocity components in an incompressible, twodimensional flow field are given by the equations \\[\begin{array}{l}u=x^{2} \\\v=-2 x y+x\end{array}\\] Determine, if possible, the corresponding stream function.
Short Answer
Expert verified
Stream function is \( \psi(x, y) = x^2 y - \frac{x^2}{2} + C \).
Step by step solution
01
Understand the Stream Function Concept
In two-dimensional, incompressible flow, the stream function \( \psi \) is related to the velocity components \( u \) and \( v \) by the equations: \( u = \frac{\partial \psi}{\partial y} \) and \( v = -\frac{\partial \psi}{\partial x} \). Our goal is to find a function \( \psi(x,y) \) that satisfies these conditions.
02
Integrate for the u Component
The velocity component \( u = x^2 \) is given. According to \( u = \frac{\partial \psi}{\partial y} \), we integrate \( u \) with respect to \( y \) to find: \[ \psi = \int x^2 \, dy = x^2 y + f(x) \] where \( f(x) \) is an arbitrary function of \( x \) only.
03
Differentiate for the v Component
The velocity component \( v = -2xy + x \) is given. According to \( v = -\frac{\partial \psi}{\partial x} \), we differentiate \( \psi = x^2 y + f(x) \) with respect to \( x \): \[ \frac{\partial \psi}{\partial x} = 2xy + f'(x) \] Setting \(-\frac{\partial \psi}{\partial x} = v\), we get: \[ - (2xy + f'(x)) = -2xy + x \]
04
Solve for the Function f(x)
From the equation \(- (2xy + f'(x)) = -2xy + x\), we infer: \[ f'(x) = -x \] Integrating with respect to \( x \) gives: \[ f(x) = -\frac{x^2}{2} + C \] where \( C \) is an arbitrary constant.
05
Assemble the Stream Function
Substitute \( f(x) = -\frac{x^2}{2} + C \) back into the expression for \( \psi \) obtained in Step 2: \[ \psi(x, y) = x^2 y + \left( -\frac{x^2}{2} \right) + C \] simplify this to: \[ \psi(x, y) = x^2 y - \frac{x^2}{2} + C \] This is the stream function satisfying the problem's conditions.
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Stream Function
In fluid mechanics, especially when dealing with two-dimensional flow, the stream function is an essential tool. It provides a way to visualize and analyze fluid flow without recourse to the use of vectors. The stream function, denoted as \( \psi \), offers a mathematical description of the flow pattern. It relates to the velocity components \( u \) and \( v \) through the equations:
- \( u = \frac{\partial \psi}{\partial y} \)
- \( v = -\frac{\partial \psi}{\partial x} \)
Velocity Components
In analyzing fluid flow, the velocity components \( u \) and \( v \) define the speed and direction of fluid particles in the flow field. Specifically, \( u \) is the component of velocity in the x-direction, and \( v \) is the component in the y-direction. For our two-dimensional flow, these are given as:
- \( u = x^2 \)
- \( v = -2xy + x \)
Two-Dimensional Flow
Fluid motion can be categorized into various dimensional forms, with two-dimensional flow being one of them. This type of flow assumes that the third dimension (usually the z-direction) has no effect on the fluid properties, making it a simplification applicable in many engineering contexts.
Two-dimensional flow occurs when changes in the fluid motion are only noticeable in a plane, typically the x-y plane. This simplification still retains much of the critical behavior of the flow while making calculations and visualizations more manageable. It provides a useful approximation for systems like air over an airfoil or water flow over a dam where lateral effects are negligible. Moreover, in computational fluid dynamics, solving two-dimensional problems requires less computational power than three-dimensional ones.
Incompressible Flow
In the realm of fluid dynamics, incompressible flow refers to a scenario where the fluid density remains constant: changes in pressure or velocity do not affect the fluid density significantly. For most liquids, this is a valid and convenient assumption. Incompressible flow simplifies the equations governing fluid behavior, as the continuity equation reduces to: \[\frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} = 0\] This mathematical condition means that the fluid's volumetric flow rate remains consistent across any cross-section of the flow. In sum, incompressible flow assumptions make solving fluid dynamics problems easier without significantly losing accuracy in many practical scenarios.