Chapter 18: Problem 7
Solve $$ \sin x \frac{\partial u}{\partial x}+\cos x \frac{\partial u}{\partial y}=\cos x $$ subject to (a) \(u(\pi / 2, y)=0\), (b) \(u(\pi / 2, y)=y(y+1)\).
Short Answer
Expert verified
Characteristic method and boundary conditions yield \(u=g(-\ln|\cot(x/2)| - \ln|\sec(y)|)\)
Step by step solution
01
Identify the type of PDE
Recognize that the given equation is a first-order linear partial differential equation (PDE).
02
Use the method of characteristics
To solve the PDE, use the method of characteristics. This involves defining characteristic equations: \[ \frac{dx}{\text{sin}(x)} = \frac{dy}{\text{cos}(x)} = \frac{du}{\text{cos}(x)} \]}, {
03
Solve the characteristic equations
Integrate each portion of the characteristic equations: \[ \int \frac{dx}{\text{sin}(x)} = \int \frac{dy}{\text{cos}(x)} \], which results in \[ -\ln|\cot(x/2)| = \ln|\sec(y)| \]
04
Combine these integrals
Combine the integrals to find a relationship between x and y: \[ -\ln|\cot(x/2)| - \ln|\sec(y)| = C \].
05
Transform into solution form
Convert the relation to return u as: \[ u = g(C) \], where g is some arbitrary function, leading to: \[ u = g(-\ln|\cot(x/2)| - \ln|\sec(y)|) \]
06
Solve for specific solutions with boundary conditions
Apply the boundary conditions: (a) \(u(\pi / 2, y)=0\): Since \(\sin(\pi/2)=1\) and \(\cos(\pi/2)=0\): Substitute to find function g\[ g(-\ln|\cot((\pi/2)/2)| - \ln|\sec(y)|) = 0 \] which simplifies to the functional form. Repeat for (b) boundary: \(u(\pi / 2, y)=y(y+1)\)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
First-Order Partial Differential Equations
First-order partial differential equations (PDEs) involve the first derivatives of the unknown function. In the given exercise, the PDE is \(\rxjsin x \frac{\partial u}{\partial x} + \cos x \frac{\partial u}{\partial y} = \cos x\). These PDEs are crucial in modeling various physical phenomena, such as heat diffusion and wave propagation. Understanding them helps in solving complex systems.
Since the PDE is first-order, it involves derivatives of the dependent variable \(u\) with respect to the independent variables \(x\) and \(y\). The term 'first-order' indicates that the highest degree of differentiation in the equation is one.
For any first-order PDE, solutions typically look for functions that satisfy the given differential relationship between the changing variables.
Since the PDE is first-order, it involves derivatives of the dependent variable \(u\) with respect to the independent variables \(x\) and \(y\). The term 'first-order' indicates that the highest degree of differentiation in the equation is one.
For any first-order PDE, solutions typically look for functions that satisfy the given differential relationship between the changing variables.
Boundary Conditions
Boundary conditions are additional constraints that a solution to a PDE must satisfy. In the given exercise, two boundary conditions are provided: (a) \(u(\frac{\pi}{2}, y)=0\) and (b) \(u(\frac{\pi}{2}, y)=y(y+1)\).
- Boundary conditions allow multiple potential solutions to be narrowed down to the one that correctly describes the physical situation.
- They define the value of the solution or its derivatives at specific points or regions, crucial for solving real-world problems.
- For instance, in thermal analysis, boundary conditions could represent the fixed temperature at the surface of an object.
Characteristic Equations
The method of characteristics transforms a PDE into a set of ordinary differential equations (ODEs) known as characteristic equations. For the given PDE, the characteristic equations are derived as follows:
\( \frac{dx}{\sin(x)} = \frac{dy}{\cos(x)} = \frac{du}{\cos(x)}\)
This link becomes significant when we apply it to find solutions that satisfy the initial boundary conditions.
\( \frac{dx}{\sin(x)} = \frac{dy}{\cos(x)} = \frac{du}{\cos(x)}\)
- These equations help us trace paths along which the PDE reduces to an ODE.
- Characteristic equations simplify solving PDEs by converting them into easier-to-handle ODEs.
- Solving these ODEs provides a relationship among the variables, forming the basis of the solution.
This link becomes significant when we apply it to find solutions that satisfy the initial boundary conditions.
Linear PDE
A PDE is termed linear if it can be expressed as a linear combination of the unknown function and its derivatives. The term 'linear' implies that the unknown function and its partial derivatives appear in a linear form, without being multiplied or divided by each other.
In the given problem, the PDE \(\rxjsin x \frac{\partial u}{\partial x} + \cos x \frac{\partial u}{\partial y} = \cos x\) is linear because \(u\) and its partial derivatives \(\frac{\partial u}{\partial x}\) and \(\frac{\partial u}{\partial y}\) appear in a linear manner.
In the given problem, the PDE \(\rxjsin x \frac{\partial u}{\partial x} + \cos x \frac{\partial u}{\partial y} = \cos x\) is linear because \(u\) and its partial derivatives \(\frac{\partial u}{\partial x}\) and \(\frac{\partial u}{\partial y}\) appear in a linear manner.
- Linear PDEs are generally easier to solve compared to nonlinear PDEs.
- Solutions to linear PDEs can often be superimposed to form more complex solutions.
- Understanding linear PDEs builds a foundation for tackling more complicated non-linear scenarios.