Problem 24
Question
Verify that the given function \(u\) is harmonic. Find \(v\), the harmonic conjugate function of \(u\). Form the corresponding analytic function \(f(z)=u+i v .\) \(u(x, y)=2 x-2 x y\)
Step-by-Step Solution
Verified Answer
The analytic function is \( f(z) = (2x - 2xy) + i(2y - y^2 - x^2 + C) \).
1Step 1: Verify Harmonic Condition
A function is harmonic if it satisfies Laplace's equation, \( abla^2 u = 0 \). For \( u(x,y) = 2x - 2xy \), calculate the second partial derivatives.\\[\frac{\partial^2 u}{\partial x^2} = \frac{\partial}{\partial x}(2-2y) = 0\]\\[\frac{\partial^2 u}{\partial y^2} = \frac{\partial}{\partial y}(-2x) = 0\]\Since \( \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0 + 0 = 0 \), \( u(x, y) \) satisfies Laplace's equation, so it is harmonic.
2Step 2: Find Harmonic Conjugate
For a harmonic function \( u(x,y) \), the harmonic conjugate \( v(x,y) \) satisfies the Cauchy-Riemann equations: \( \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \) and \( \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x} \).Calculate \( \frac{\partial u}{\partial x} = 2 - 2y \) and \( \frac{\partial u}{\partial y} = -2x \).1. From \( \frac{\partial v}{\partial y} = 2 - 2y \): Integrate with respect to \( y \) to find \( v \): \[ v(x,y) = 2y - y^2 + g(x) \] \2. From \( \frac{\partial v}{\partial x} = -2x \): \[ \frac{\partial}{\partial x}(2y - y^2 + g(x)) = g'(x) = -2x \] \ Integrate to find \( g(x) \): \ \[ g(x) = - x^2 + C \] \So, \( v(x,y) = 2y - y^2 - x^2 + C \).
3Step 3: Form the Analytic Function
The analytic function \( f(z) \) is formed by combining the harmonic function \( u(x,y) \) and its conjugate \( v(x,y) \):\[ f(z) = u(x,y) + iv(x,y) = (2x - 2xy) + i(2y - y^2 - x^2 + C) \].
Key Concepts
Laplace's equationHarmonic ConjugateCauchy-Riemann equations
Laplace's equation
Laplace's equation is a second-order partial differential equation essential in mathematical physics. It is represented as \( abla^2 u = 0 \), meaning the sum of the second partial derivatives of a function \( u \) with respect to the variables is zero. This equation characterizes harmonic functions, which are solutions to this equation.
For a function \( u(x, y) \) to be harmonic, it must satisfy this equation in the given domain. In the context of our exercise, the function \( u(x, y) = 2x - 2xy \) was checked against Laplace's equation.
By calculating the second partial derivatives, \( \frac{\partial^2 u}{\partial x^2} = 0 \) and \( \frac{\partial^2 u}{\partial y^2} = 0 \), it was verified that their sum is zero. Hence, \( u(x, y) \) is indeed a harmonic function because it fulfills \( abla^2 u = 0 \).
Harmonic functions have many applications in physics, such as in the modeling of electrostatic potential and fluid dynamics, as they often represent equilibrium states. Learning about Laplace's equation is crucial for understanding complex occurred phenomena in these fields.
For a function \( u(x, y) \) to be harmonic, it must satisfy this equation in the given domain. In the context of our exercise, the function \( u(x, y) = 2x - 2xy \) was checked against Laplace's equation.
By calculating the second partial derivatives, \( \frac{\partial^2 u}{\partial x^2} = 0 \) and \( \frac{\partial^2 u}{\partial y^2} = 0 \), it was verified that their sum is zero. Hence, \( u(x, y) \) is indeed a harmonic function because it fulfills \( abla^2 u = 0 \).
Harmonic functions have many applications in physics, such as in the modeling of electrostatic potential and fluid dynamics, as they often represent equilibrium states. Learning about Laplace's equation is crucial for understanding complex occurred phenomena in these fields.
Harmonic Conjugate
A harmonic conjugate is another function that pairs with a given harmonic function to form an analytic function. In this context, when a function \( u(x, y) \) is harmonic, it pairs with its conjugate \( v(x, y) \) to create the complex function \( f(z) = u(x, y) + iv(x, y) \). This means \( f(z) \) becomes analytic at that point.
To find the harmonic conjugate, we use the Cauchy-Riemann equations, which must be satisfied by \( u \) and \( v \):
In the exercise, \( \frac{\partial u}{\partial x} = 2 - 2y \) and \( \frac{\partial u}{\partial y} = -2x \) were calculated, leading to the conclusion that \( v(x, y) = 2y - y^2 - x^2 + C \).
This procedure of finding \( v \) complements \( u \), fulfilling its role as a harmonic conjugate, which is key for forming the analytic function and understanding complex mapping.
To find the harmonic conjugate, we use the Cauchy-Riemann equations, which must be satisfied by \( u \) and \( v \):
- \( \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \)
- \( \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x} \)
In the exercise, \( \frac{\partial u}{\partial x} = 2 - 2y \) and \( \frac{\partial u}{\partial y} = -2x \) were calculated, leading to the conclusion that \( v(x, y) = 2y - y^2 - x^2 + C \).
This procedure of finding \( v \) complements \( u \), fulfilling its role as a harmonic conjugate, which is key for forming the analytic function and understanding complex mapping.
Cauchy-Riemann equations
The Cauchy-Riemann equations are foundational in complex analysis, establishing the conditions under which a complex function is analytic. They interrelate the partial derivatives of two real-valued functions, \( u(x, y) \) and \( v(x, y) \), which together form a complex number, \( z = x + iy \). These equations boil down to:
These must be satisfied for \( u \) and \( v \) to form a valid analytic function \( f(z) = u(x, y) + iv(x, y) \).
In the exercise, these equations were employed to verify the harmonic nature of \( u \) and to find \( v \), its conjugate, ensuring \( f(z) \) is analytic. By satisfying these equations, you confirm that \( f(z) \) behaves nicely, particularly in the domain of complex analysis, enabling smooth, differentiable behavior.
Understanding how to apply Cauchy-Riemann is crucial, not just for theoretical exploration but also for practical applications, such as solving fluid dynamics problems and analyzing electromagnetic fields.
- \( \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \)
- \( \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x} \)
These must be satisfied for \( u \) and \( v \) to form a valid analytic function \( f(z) = u(x, y) + iv(x, y) \).
In the exercise, these equations were employed to verify the harmonic nature of \( u \) and to find \( v \), its conjugate, ensuring \( f(z) \) is analytic. By satisfying these equations, you confirm that \( f(z) \) behaves nicely, particularly in the domain of complex analysis, enabling smooth, differentiable behavior.
Understanding how to apply Cauchy-Riemann is crucial, not just for theoretical exploration but also for practical applications, such as solving fluid dynamics problems and analyzing electromagnetic fields.
Other exercises in this chapter
Problem 24
Prove that \(\sinh z=\sinh x \cos y+i \cosh x \sin y\)
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Express \(\ln z\) in the form \(a+i b\). \(z=-e i\)
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In Problems 21-24, sketch the set of points in the complex plane satisfying the given inequality. $$ \operatorname{Im}(z)
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In Problems 23-28, express \(\ln z\) in the form \(a+i b\). \(z=-e i\)
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