Problem 11
Question
Set up the boundary-value problem for the steady-state temperature \(u(x, y)\). A thin rectangular plate coincides with the region in the \(x y\) -plane defined by \(0 \leq x \leq 4,0 \leq y \leq 2\). The left end and the bottom of the plate are insulated. The top of the plate is held at temperature zero, and the right end of the plate is held at temperature \(f(y)\).
Step-by-Step Solution
Verified Answer
The boundary-value problem involves the Laplace equation with given boundary conditions on a rectangular domain.
1Step 1: Define the Domain
The domain of the problem is a rectangle in the \(xy\)-plane, given by \(0 \leq x \leq 4\) and \(0 \leq y \leq 2\).
2Step 2: State the Differential Equation
Since the problem involves finding the steady-state temperature, the governing equation is the Laplace equation: \[ \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0. \]
3Step 3: Set the Boundary Conditions
In order to find a unique solution, we specify boundary conditions:- Left end and bottom are insulated: \( \frac{\partial u}{\partial x} \bigg|_{x=0} = 0\) and \( \frac{\partial u}{\partial y} \bigg|_{y=0} = 0\).- Top is held at temperature zero: \( u(x, 2) = 0 \) for \(0 \leq x \leq 4\).- Right end is held at temperature \(f(y)\): \( u(4, y) = f(y) \) for \(0 \leq y \leq 2\).
4Step 4: Formulate the Boundary-Value Problem
The boundary-value problem is to find a function \(u(x, y)\) such that:- \( \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0\) for \(0 < x < 4\) and \(0 < y < 2\).- Subject to the boundary conditions: - \( \frac{\partial u}{\partial x} \bigg|_{x=0} = 0\), - \( \frac{\partial u}{\partial y} \bigg|_{y=0} = 0\), - \( u(x, 2) = 0 \), - \( u(4, y) = f(y) \).
Key Concepts
Laplace EquationSteady-State TemperaturePartial Differential Equations
Laplace Equation
The Laplace Equation is a second-order partial differential equation. It appears often in fields such as physics and engineering. This equation is used to describe many physical phenomena, including electrostatics, fluid flow, and steady-state heat conduction like in the current problem. The general form of the Laplace Equation in two dimensions is:\[\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0\]
- \(u\) represents a function whose behavior we want to predict. It's the temperature distribution in this context.
- \(\frac{\partial^2 u}{\partial x^2}\) and \(\frac{\partial^2 u}{\partial y^2}\) indicate the second partial derivatives concerning \(x\) and \(y\), respectively.
- The sum of these derivatives equaling zero signifies a steady state where temperature does not change over time.
Steady-State Temperature
Steady-state temperature refers to a condition where the temperature distribution remains constant over time. When a system reaches this state, the heat entering any point in the system equals the heat leaving that point. In such scenarios, heat flow has balanced perfectly. In the given problem, we're examining a rectangular plate, asking how the temperature stabilizes.
- For steady-state temperature, the distribution function \(u(x, y)\) does not change with time.
- The governing equation, in this case, is the Laplace Equation, reflecting the balance of heat.
- Boundary conditions are crucial: parts of the plate are insulated, and specific sections are maintained at constant temperatures like zero or \(f(y)\).
Partial Differential Equations
Partial Differential Equations (PDEs) are equations that involve rates of change with respect to continuous variables. These equations are vital in modeling how physical quantities vary in space and time. PDEs like the Laplace Equation are particularly useful in multi-dimensional situations.Key characteristics of PDEs include:
- They contain unknown multivariable functions and their partial derivatives.
- PDEs are essential in fields such as physics, engineering, and finance.
- Solving PDEs often involves numerical methods and approximation due to their complexity.
Other exercises in this chapter
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