Problem 21
Question
Classify the given partial differential equation as hyperbolic, parabolic, or elliptic.\(\frac{\partial^{2} u}{\partial x^{2}}=9 \frac{\partial^{2} u}{\partial x \partial y}\)
Step-by-Step Solution
Verified Answer
The equation is hyperbolic since \( \Delta = 81 > 0 \).
1Step 1: Identify the General Form
A second-order linear partial differential equation can usually be identified by its general form: \( A \frac{\partial^2 u}{\partial x^2} + B \frac{\partial^2 u}{\partial x \partial y} + C \frac{\partial^2 u}{\partial y^2} = 0 \). In our equation, \( A = 1 \), \( B = -9 \), and \( C = 0 \), given by \( \frac{\partial^{2} u}{\partial x^{2}}=9 \frac{\partial^{2} u}{\partial x \partial y} \).
2Step 2: Evaluate the Discriminant
For classification, calculate the discriminant \( \Delta = B^2 - 4AC \). Substitute the identified coefficients to get \( \Delta = (-9)^2 - 4 \cdot 1 \cdot 0 = 81 - 0 = 81 \).
3Step 3: Classify Based on Discriminant Value
Compare the discriminant with zero: if \( \Delta > 0 \), it is hyperbolic; if \( \Delta = 0 \), it is parabolic; if \( \Delta < 0 \), it is elliptic. Since \( \Delta = 81 \), and \( 81 > 0 \), the equation is classified as hyperbolic.
Key Concepts
Hyperbolic EquationsDiscriminant EvaluationSecond-Order Linear PDE Classification
Hyperbolic Equations
In the world of partial differential equations (PDEs), hyperbolic equations hold a special distinction by presenting themselves with dynamic structures. Such equations are well-suited for describing wave phenomena, among other things, and generally possess solutions that propagate along characteristic lines. These characteristic lines are particular paths in the plane where information travels consistently.
Hyperbolic PDEs are identified based on the value of their discriminant, always being greater than zero. This attribute is intrinsically linked to the nature of the solutions they produce. When the discriminant is positive, it allows for two distinct real roots, which translates into real characteristics, pivotal for explaining physical phenomena like sound waves or vibrations. Thus, in regions of practical application, hyperbolic equations enable us to model events where distinct signals can travel in different directions without intersecting each other.
The classic wave equation is a quintessential example of a hyperbolic PDE. Understanding these types of equations is crucial for disciplines involving any form of wave mechanics, be it in acoustics, electromagnetism, or fluid dynamics.
Hyperbolic PDEs are identified based on the value of their discriminant, always being greater than zero. This attribute is intrinsically linked to the nature of the solutions they produce. When the discriminant is positive, it allows for two distinct real roots, which translates into real characteristics, pivotal for explaining physical phenomena like sound waves or vibrations. Thus, in regions of practical application, hyperbolic equations enable us to model events where distinct signals can travel in different directions without intersecting each other.
The classic wave equation is a quintessential example of a hyperbolic PDE. Understanding these types of equations is crucial for disciplines involving any form of wave mechanics, be it in acoustics, electromagnetism, or fluid dynamics.
Discriminant Evaluation
The discriminant in the context of second-order PDEs is akin to a powerful tool that unlocks the classification of these equations. It offers clarity by mathematically determining the nature of the equation, based on the values and signs of its coefficients. By evaluating the discriminant, we can distinguish between hyperbolic, parabolic, and elliptic equations in a straightforward manner.
The discriminant \[ \Delta = B^2 - 4AC \] gets computed by substituting the values of coefficients A, B, and C from the PDE. These coefficients come from the general form \[ A \frac{\partial^2 u}{\partial x^2} + B \frac{\partial^2 u}{\partial x \partial y} + C \frac{\partial^2 u}{\partial y^2} = 0. \]
The discriminant \[ \Delta = B^2 - 4AC \] gets computed by substituting the values of coefficients A, B, and C from the PDE. These coefficients come from the general form \[ A \frac{\partial^2 u}{\partial x^2} + B \frac{\partial^2 u}{\partial x \partial y} + C \frac{\partial^2 u}{\partial y^2} = 0. \]
- If \( \Delta > 0 \), it reveals a hyperbolic nature.
- If \( \Delta = 0 \), it points to a parabolic type of equation.
- If \( \Delta < 0 \), it indicates an elliptic classification.
Second-Order Linear PDE Classification
Classification of second-order linear partial differential equations is a systematic method to understand the behavior and solution characteristics of these mathematical expressions. It allows mathematicians and physicists to discern how solutions spread out over time and space.
To classify a second-order linear PDE, it’s essential to express it in its canonical form: \[ A \frac{\partial^2 u}{\partial x^2} + B \frac{\partial^2 u}{\partial x \partial y} + C \frac{\partial^2 u}{\partial y^2} = 0. \]With this general representation, assignments follow:
To classify a second-order linear PDE, it’s essential to express it in its canonical form: \[ A \frac{\partial^2 u}{\partial x^2} + B \frac{\partial^2 u}{\partial x \partial y} + C \frac{\partial^2 u}{\partial y^2} = 0. \]With this general representation, assignments follow:
- Identify and designate the appropriate coefficients A, B, and C from the equation.
- Apply the discriminant formula \( \Delta = B^2 - 4AC \).
- Classify according to the discriminant's result: hyperbolic (\(\Delta > 0\)), parabolic (\(\Delta = 0\)), or elliptic (\(\Delta < 0\)).
Other exercises in this chapter
Problem 21
Solve the Neumann problem for a rectangle: $$ \begin{aligned} &\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}=0,0
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Consider the boundary-value problem $$ \begin{aligned} &\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}=0,0
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Classify the given partial differential equation as hyperbolic, parabolic, or elliptic.\(\frac{\partial^{2} u}{\partial x^{2}}+2 \frac{\partial^{2} u}{\partial
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