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Consider the eigenvalues given by equation ( 39 ). Show that $$\left(\sigma_{1} X+\sigma_{2} Y\right)^{2}-4\left(\sigma_{1} \sigma_{2}-\alpha_{1} \alpha_{2}\right) X Y=\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} X Y$$ Hence conclude that the eigenvalues can never be complex-valued.

Short Answer

Expert verified
Question: Prove that the eigenvalues cannot be complex-valued for the given expression: $$(\sigma_{1} X+\sigma_{2} Y)^{2}-4(\sigma_{1}\sigma_{2}-\alpha_{1} \alpha_{2}) XY=\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} XY$$ Answer: We have shown that the given expression is equal to the expression $$\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} XY$$ which has squared terms and no terms with imaginary numbers. This implies the eigenvalues cannot be complex-valued since the square root of a positive number (or zero) cannot result in a complex number. Thus, the eigenvalues are real numbers.

Step by step solution

01

Given expression

We first write down the given expression $$(\sigma_{1} X+\sigma_{2} Y)^{2}-4(\sigma_{1}\sigma_{2}-\alpha_{1} \alpha_{2}) XY=\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} XY$$
02

Expand the expression

We will now expand both sides of the equation. The left-hand side expansion: $$\left(\sigma_{1} X+\sigma_{2} Y\right)^{2}-4(\sigma_{1}\sigma_{2}-\alpha_{1} \alpha_{2}) XY = \sigma_{1}^2X^2 + 2\sigma_{1}\sigma_{2}XY + \sigma_{2}^2Y^2 - 4\sigma_{1}\sigma_{2}XY + 4\alpha_{1}\alpha_{2}XY$$ The right-hand side expansion: $$\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} XY = \sigma_{1}^2X^2 - 2\sigma_{1}\sigma_{2}XY + \sigma_{2}^2Y^2 + 4\alpha_{1}\alpha_{2} XY$$
03

Comparing the expanded expressions

Comparing both expanded expressions, we see they have the same terms and hence are equal: $$\sigma_{1}^2X^2 + 2\sigma_{1}\sigma_{2}XY + \sigma_{2}^2Y^2 - 4\sigma_{1}\sigma_{2}XY + 4\alpha_{1}\alpha_{2}XY = \sigma_{1}^2X^2 - 2\sigma_{1}\sigma_{2}XY + \sigma_{2}^2Y^2 + 4\alpha_{1}\alpha_{2} XY$$
04

Concluding the eigenvalues are not complex-valued

The given expression is shown to be equal to the target expression, which has the form: $$\left(\sigma_{1} X-\sigma_{2} Y\right)^{2}+4 \alpha_{1} \alpha_{2} XY$$ This expression contains squared terms and none with imaginary numbers. Therefore, the eigenvalues cannot be complex-valued since the square root of a positive number (or zero) cannot result in a complex number. Hence, the eigenvalues are real numbers.

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Key Concepts

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

Understanding Differential Equations
Differential equations are mathematical equations that describe the relationship between a function and its derivatives. They play a central role in mathematics, physics, engineering, and other sciences, as they represent processes where change is involved. For instance, they can describe how the position of a moving particle changes over time or how heat diffuses through a material.

In the context of the given exercise, differential equations may arise when dealing with physical systems that can be represented by eigenvalues and eigenvectors. Eigenvalues are particularly important in the solution of linear differential equations, as they can provide insights into the behavior of the system, such as its stability and oscillation frequencies.

When a system can be described by a set of differential equations, finding the eigenvalues allows us to solve these equations more easily, especially when they are linear. An eigenvalue problem in a differential equation context involves finding solutions, typically nontrivial ones, that satisfy both the differential equation and certain boundary conditions. To determine if a system has complex solutions, one usually checks the discriminant of a corresponding characteristic equation, which can often be related to eigenvalues.
Exploring Boundary Value Problems
Boundary value problems (BVPs) are a type of differential equation where the solution is defined not only by the differential equation itself but also by the specified values, or boundaries, the solution must satisfy. These boundaries can be initial values at certain points, or conditions at the edges of an interval for spatial problems.

In the exercise, understanding whether eigenvalues can be complex is critical, especially when the eigenvalues are used to solve boundary value problems. The presence of complex eigenvalues in BVPs can indicate a system that has oscillatory or wave-like solutions, while real eigenvalues typically correspond to non-oscillatory behavior.

Eigenvalues being real indicates that the associated eigenfunctions will satisfy the BVP without leading to growing or decaying oscillations, which could violate the boundary conditions. It's important for students to recognize that eigenvalues play a significant role in defining the nature of solutions to boundary value problems in differential equations.
The Intersection of Linear Algebra
Linear algebra is the branch of mathematics concerning linear equations, linear functions, and their representations in vector spaces and through matrices. Eigenvalues are a fundamental concept in linear algebra, where they characterize important properties of linear transformations.

Solving Systems Using Eigenvalues

The eigenvalues of a matrix can tell us whether systems of linear equations have unique solutions, infinite solutions, or no solutions at all. This is deeply connected to the concepts addressed in the exercise.

Understanding Matrix Behavior

Eigenvalues also inform us about the scaling and rotation operations of a matrix, which can be critical when analyzing differential equations that model dynamic systems.

Additionally, eigenvalues come into play in various applications, such as stability analysis, where real eigenvalues, especially those which are not complex, indicate a stable or uncontrollable system depending on their sign. In the context of our exercise, by demonstrating that the eigenvalues are real, we're asserting that the solutions to the system will not exhibit complex behaviors, like oscillations, and remain within the realm of real numbers.

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Most popular questions from this chapter

As mentioned in the text, one improvement in the predator-prey model is to modify the equation for the prey so that it has the form of a logistic equation in the absence of the predator. Thus in place of Eqs. ( 1 ) we consider the system $$ d x / d t=x(a-\sigma x-\alpha y), \quad d y / d t=y(-c+\gamma x) $$ where \(a, \sigma, \alpha, c,\) and \(\gamma\) are positive constants. Determine all critical points and discuss their nature and stability characteristics. Assume that \(a / \sigma \gg c / \gamma .\) What happens for initial data \(x \neq 0, y \neq 0 ?\)

The system \\[ x^{\prime}=-y, \quad y^{\prime}=-\gamma y-x(x-0.15)(x-2) \\] results from an approximation to the Hodgkin-Huxley \(^{6}\) equations, which model the transmission of neural impulses along an axon. a. Find the critical points, and classify them by investigating the approximate linear system near each one. b. Draw phase portraits for \(\gamma=0.8\) and for \(\gamma=1.5\) c. Consider the trajectory that leaves the critical point (2, 0). Find the value of \(\gamma\) for which this trajectory ultimately approaches the origin as \(t \rightarrow \infty .\) Draw a phase portrait for this value of \(\gamma\).

(a) Find all the critical points (equilibrium solutions). (b) Use a computer to draw a direction field and portrait for the system. (c) From the plot(s) in part (b) determine whether each critical point is asymptotically stable, stable, or unstable, and classify it as to type. $$ \text { The van der Pol equation: } \quad d x / d t=y, \quad d y / d t=\left(1-x^{2}\right) y-x $$

(a) Find an equation of the form \(H(x, y)=c\) satisfied by the trajectories. (b) Plot several level curves of the function \(H\). These are trajectories of the given system. Indicate the direction of motion on each trajectory. $$ d x / d t=2 y, \quad d y / d t=-8 x $$

The system $$ x^{\prime}=3\left(x+y-\frac{1}{5} x^{3}-k\right), \quad y^{\prime}=-\frac{1}{3}(x+0.8 y-0.7) $$ is a special case of the Fitahugh-Nagumo equations, which model the transmission of neural impulses along an axon. The parameter \(k\) is the external stimulus. (a) For \(k=0\) show that there is one critical point. Find this point and show that it is an asymptotically stable spiral point. Repeat the analysis for \(k=0.5\) and show the critical point is now an unstable spiral point. Draw a phase portrait for the system in each case. (b) Find the value \(k_{0}\) where the critical point changes from asymptotically stable to unstable. Draw a phase portrait for the system for \(k=k_{0}\). (c) For \(k \geq k_{0}\) the system exhibits an asymptotically stable limit cycle. Plot \(x\) versus \(t\) for \(k=k_{0}\) for several periods and estimate the value of the period \(T\). (d) The limit cycle actually exists for a small range of \(k\) below \(k_{0}\). Let \(k_{1}\) be the smallest value of \(k\) for which there is a limit cycle. Find \(k_{1}\).

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