/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 26 Compute the circulation and net ... [FREE SOLUTION] | 91Ó°ÊÓ

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Compute the circulation and net flux for the given flow and the indicated closed contour \(C\). \(f(z)=2 z ;\) where \(C\) is the circle \(|z|=1\)

Short Answer

Expert verified
Both the circulation and net flux are 0.

Step by step solution

01

Understanding the Flow Function

The given complex function is \( f(z) = 2z \). In terms of complex analysis, \( f(z) \) is used to determine the flow. We need to compute attributes related to this flow on a specific contour.
02

Identifying the Contour

The contour \( C \) is given as the circle \( |z| = 1 \). This means that the contour is a unit circle and has the parametric form \( z(t) = e^{it} \) for \( t \in [0, 2\pi] \).
03

Circulation Calculation

The circulation of a vector field along a closed path \( C \) is given by \( \oint_{C} f(z) \; dz \). For \( f(z) = 2z \), the integral becomes \( \oint_{C} 2z \; dz \). Substituting \( z(t) = e^{it} \) and \( dz = i e^{it} dt \), the integral becomes: \[ \int_{0}^{2\pi} 2e^{it} (i e^{it}) dt = 2i \int_{0}^{2\pi} e^{2it} dt \]. Now, compute this integral: \[ 2i \int_{0}^{2\pi} e^{2it} dt = 2i \left[ \frac{e^{2it}}{2i} \right]_0^{2\pi} = e^{2i(2\pi)} - e^{2i(0)} = 1 - 1 = 0 \]. Thus, the circulation is 0.
04

Net Flux Using Cauchy-Goursat Theorem

Since \( f(z) \) is a holomorphic (analytic) function where \( |z| = 1 \), the net flux through the contour can be found using the Cauchy-Goursat theorem. In particular, because the function is entire and there are no singularities within or on \( |z| = 1 \), the net flux (integral over \( C \)) is 0.

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Key Concepts

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

Circulation
In complex analysis, circulation refers to the line integral of a vector field around a closed curve. For a given complex function, it measures how much the field "circulates" around the path.
When the path is a closed contour, as in our problem, the circulation is determined by the contour integral:
  • Express the circulation formula as \(\oint_{C} f(z)\,dz\).
  • For the problem at hand, where \( f(z)=2z \) and the contour is a unit circle \( |z|=1 \), we transform the function using \( z(t) = e^{it} \) to make it easier to integrate.
Once we have the integrand in terms of \(t\), we calculate the integral from \(0\) to \(2\pi\), the complete range for a circle.
This straightforward approach reveals that the integral simplifies to \(0\), hence the circulation is zero.
This particular result emphasizes that the vector field \(2z\) produces no net rotation around the unit circle.
Net Flux
Net flux in complex analysis is concerned with the "flow" through a particular region enclosed by a path. While circulation measures flow around a path, net flux measures flow across a boundary into or out of a region.
To find the net flux, we evaluate the integral \(\oint_{C} f(z)\,dz\) across the closed contour \(C\).
In this case with \( f(z)=2z \) and \( |z|=1 \), we employ the properties of holomorphic functions. Here comes the Cauchy-Goursat theorem to the rescue.
The theorem states that for an analytic function without singularities inside or on the contour, this contour integral equals zero. Thus, the net flux is confirmed to be zero.
This result indicates that there is no net outward or inward flow through the boundary defined by the contour.
Contour Integration
Contour integration is a fundamental concept for evaluating integrals in the complex plane. It involves integrating a complex function over a path, called a contour, which can be any curve in the complex plane.
Our exercise helps demonstrate contour integration through a specific contour, the unit circle \(|z|=1\), with a function \( f(z)=2z \).
We want to integrate this over the whole circle, for which we parameterize using \(z(t)=e^{it}\). This allows the integration over the circle to be conducted in terms of \(t\), from \(0\) to \(2\pi\).
Through this process, we gain insights about how complex functions behave around particular paths.
  • This tool becomes particularly powerful for evaluating integrals around contours in complex number scenarios.
  • It also helps solve real-world problems where an understanding of how quantities circulate or flux over regions is required.
Cauchy-Goursat Theorem
The Cauchy-Goursat Theorem is one of the central results in complex analysis. It states that if a function is holomorphic (analytic) within and on a simple closed contour, then the line integral of the function around the contour is zero.
The understanding is crucial for both mathematical insight and practical applications.
For our exercise:
  • The complex function \( f(z)=2z \) is entire, meaning it is holomorphic everywhere, and specifically on the contour \(|z|=1\).
  • The function has no singularities within or on the contour, qualifying it for the theorem's conditions.
Relying on the Cauchy-Goursat theorem, we directly deduce that both the circulation and net flux are zero.
This reflects not just an integral property, but also the harmonious behavior of analytic functions over paths in the complex plane.
In many cases, the theorem allows us to avoid complex computations by directly applying the result where conditions are met.

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Most popular questions from this chapter

The flow described by the velocity field \(f(z)=(a+i b) / \bar{z}\) is said to have a vortex at \(z=0 .\) The geometric nature of the streamlines depends on the choice of \(a\) and \(b\). (a) Show that if \(z(t)=x(t)+i y(t)\) is the path of a particle in the flow, then $$ \begin{aligned} &\frac{d x}{d t}=\frac{a x-b y}{x^{2}+y^{2}} \\ &\frac{d y}{d t}=\frac{b x+a y}{x^{2}+y^{2}} \end{aligned} $$ (b) Rectangular and polar coordinates are related by \(r^{2}=x^{2}+y^{2}\), tan \(\theta=y / x\). Use these equations to show that $$ \frac{d r}{d t}-\frac{1}{r}\left(x \frac{d x}{d t}+y \frac{d y}{d t}\right), \frac{d \theta}{d t}-\frac{1}{r^{2}}\left(-y \frac{d x}{d t}+x \frac{d y}{d t}\right) $$ (c) Use the equations in parts (a) and (b) to establish that $$ \frac{d r}{d t}=\frac{a}{r}, \frac{d \theta}{d t}=\frac{b}{r^{2}} $$ (d) Use the equations in part (c) to conclude that the streamlines of the flow are logarithmic spirals \(r=c e^{a \theta / b}, b \neq 0 .\) Use a graphing utility to verify that a particle traverses a path in a counterclockwise direction if and only if \(a<0\), and in a clockwise direction if and only if \(b<0 .\) Which of these directions corresponds to motion spiraling into the vortex?

Find the velocity field \(\mathbf{F}(x, y)\) of the flow of an ideal fluid determined by the given analytic function \(g(z)\). $$ g(z)=e^{x} \cos y+i e^{x} \sin y $$

Evaluate the definite integral. If necessary, review the techniques of integration in your calculus text. $$ \int_{0}^{\pi / 8} \sec ^{2} 2 x d x $$

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Use any of the results in this section to evaluate the given integral along the indicated closed contour(s). $$ \oint_{C} \frac{1}{z^{3}+2 i z^{2}} d z ;|z|=1 $$

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