Chapter 3: Problem 21
If \(y_{1}\) and \(y_{2}\) are linearly independent solutions of \(t^{2} y^{\prime \prime}-2 y^{\prime}+(3+t) y=0\) and if \(W\left(y_{1}, y_{2}\right)(2)=3,\) find the value of \(W\left(y_{1}, y_{2}\right)(4)\)
Short Answer
Expert verified
Based on the given second-order linear differential equation and Abel's theorem, we find that the value of the Wronskian W(y_1, y_2)(4) is equal to 3/4.
Step by step solution
01
Define the given differential equation and Wronskian
We are given the second-order linear differential equation: $$t^{2} y^{\prime \prime}-2 t y^{\prime}+(3+t) y=0.$$
And we know that \(y_1(t)\) and \(y_2(t)\) are linearly independent solutions of this equation. The Wronskian \(W(y_1, y_2)\) is defined as: $$W(y_1, y_2)(t) = y_1(t)y_2'(t) - y_1'(t)y_2(t).$$
02
Applying Abel's theorem to the differential equation
Abel's theorem states that for a second-order linear homogeneous differential equation, $$p(t)y'' + q(t)y' + r(t)y = 0, $$ the Wronskian can be found by: $$W(y_1, y_2)(t) = W(y_1, y_2)(t_0) \cdot e^{-\int_{t_0}^{t} \frac{q(s)}{p(s)} ds}.$$
In our case, \(p(t) = t^2\), \(q(t) = -2t\), and \(r(t) = 3+t\). So, the expression in the integral becomes, \(\frac{-2t}{t^2} = -\frac{2}{t}\).
03
Calculate the integral in Abel's theorem
We need to calculate the integral $$-\int_{t_0}^{t} \frac{2}{s} ds$$. This evaluates to: $$-2(\ln(t) - \ln(t_0)) = -2(\ln(\frac{t}{t_0}))$$.
04
Apply Abel's theorem to find the Wronskian for any t
Now, applying Abel's theorem with the calculated integral, we have: $$W(y_1, y_2)(t) = W(y_1, y_2)(t_0) \cdot e^{-2(\ln(\frac{t}{t_0}))}$$. We are given that \(W(y_1, y_2)(2) = 3\). Let's substitute \(t_0=2\) and \(t=4\) to find \(W(y_1, y_2)(4)\).
05
Find the value of the Wronskian at t = 4
Using \(t_0=2\), \(t=4\), and \(W(y_1, y_2)(2) = 3\), we get: $$W(y_1, y_2)(4) = 3 \cdot e^{-2(\ln(\frac{4}{2}))} = 3 \cdot e^{-2(\ln(2))} = 3 \cdot \frac{1}{4}.$$ Finally, we have: $$W(y_1, y_2)(4) = \frac{3}{4}.$$
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Linear Independence
Linear independence is a fundamental concept in linear algebra and calculus. It refers to a set of functions or vectors where no member of the set can be written as a linear combination of others. In the context of differential equations, if two functions, say \(y_1(t)\) and \(y_2(t)\), are solutions to a differential equation, they are called linearly independent if the only way to weigh them, without canceling their effect entirely, is to use zero coefficients.
- This concept ensures that each function contributes its unique behavior to the solution of a differential equation.
- A basis of solutions to a differential equation, for instance, usually involves linearly independent functions to represent a wide range of phenomena.
Wronskian
The Wronskian is a determinant used to test for linear independence of functions. For two functions \(y_1(t)\) and \(y_2(t)\), their Wronskian \(W(y_1, y_2)(t)\) is defined as:\[W(y_1, y_2)(t) = y_1(t)y_2'(t) - y_1'(t)y_2(t).\]
- If the Wronskian is non-zero for some interval, the functions are linearly independent on that interval.
- It helps mathematicians verify if solutions to a differential equation are linearly independent, even if the solutions themselves aren't explicitly calculated.
Abel's Theorem
Abel's Theorem is a crucial tool when dealing with second-order linear homogeneous differential equations. This theorem provides a way to calculate the Wronskian of two solutions without needing to know the solutions explicitly. For a second-order differential equation, given by:\[p(t) y'' + q(t) y' + r(t) y = 0,\]Abel's Theorem states that:\[W(y_1, y_2)(t) = W(y_1, y_2)(t_0) \cdot e^{-\int_{t_0}^{t} \frac{q(s)}{p(s)} ds}.\]
- It's particularly useful because it turns the problem of checking linear independence into an integration problem.
- This approach avoids the more complex task of solving the differential equation directly, leveraging the simplicity of exponential functions.
Second-Order Linear Homogeneous Differential Equation
A second-order linear homogeneous differential equation is a type of differential equation characterized by a linear operator applied twice to a function. Consider equations of the form:\[t^2 y'' - 2t y' + (3 + t) y = 0.\]
- The term 'second-order' signifies the highest derivative of the function is two.
- 'Homogeneous' indicates there are no additional terms added to the equation. Usually, the solutions to these equations are functions that best describe a system's behavior in response to no external inputs.