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(a) Determine a suitable form for \(Y(t)\) if the method of undetermined coefficients is to be used. (b) Use a computer algebra system to find a particular solution of the given equation. $$ y^{\prime \prime}+4 y=t^{2} \sin 2 t+(6 t+7) \cos 2 t $$

Short Answer

Expert verified
Question: Determine the particular solution Yp(t) for the given second-order non-homogeneous linear differential equation: $$ y^{\prime \prime}+4 y=t^{2} \sin 2 t+(6 t+7) \cos 2 t $$ Answer: The particular solution Yp(t) for the given differential equation is: $$ Y_p(t) = (\frac{1}{4}t^2 + \frac{1}{2}t + \frac{1}{4}) \sin(2t) + (\frac{3}{2}t + 2) \cos(2t) $$

Step by step solution

01

Identify the differential equation

We are given the second-order non-homogeneous linear differential equation: $$ y^{\prime \prime}+4 y=t^{2} \sin 2 t+(6 t+7) \cos 2 t $$
02

Determine a suitable form for Y(t)

We will use the method of undetermined coefficients to determine a suitable form for Y(t). Since the non-homogeneous part contains a polynomial function multiplied by sine and cosine functions, we will assume a solution of the form: $$ Y(t) = (A t^2 + B t + C) \sin(2t) + (D t^2 + E t + F) \cos(2t) $$
03

Determine the first and second derivative of Y(t)

Now, we will find the first and second derivative of Y(t) with respect to t: First derivative: $$ Y'(t) = 2 (B t + 2 A t - C) \cos(2t) - 2 (E t + 2 D t - F) \sin(2t) $$ Second derivative: $$ Y^{\prime \prime}(t) = - 4 (2 A t + B) \sin(2t) - 4 (2 D t + E) \cos(2t) $$
04

Substitute Y(t), Y'(t) and Y''(t) into the given differential equation

Now we will substitute Y(t), Y'(t), and Y''(t) into the given differential equation: $$ - 4 (2 A t + B) \sin(2t) - 4 (2 D t + E) \cos(2t) + 4((A t^2 + B t + C) \sin(2t) + (D t^2 + E t + F) \cos(2t)) = t^{2} \sin 2 t+(6 t+7) \cos 2 t $$
05

Compare the coefficients

Now, we will compare the coefficients for the sine and cosine terms: For the sine terms: $$ - 8 A t -4 B + 4A t^2 + 4B t + 4C = t^2 $$ For the cosine terms: $$ - 8 D t -4 E + 4D t^2 + 4E t + 4F = 6t + 7 $$ We have the following system of equations: 1. \(4A = 1\) 2. \(4B - 8A = 0\) 3. \(4C - 4B = 0\) 4. \(4D = 0\) 5. \(4E - 8D = 6\) 6. \(4F - 4E = 7\)
06

Solve the system of equations

Solving the system of equations, we get the following values: $$ A = \frac{1}{4} $$ $$ B = \frac{1}{2} $$ $$ C = \frac{1}{4} $$ $$ D = 0 $$ $$ E = \frac{3}{2} $$ $$ F = 2 $$
07

Write the particular solution Yp(t)

Now we will write the particular solution Yp(t) using the obtained values: $$ Y_p(t) = (\frac{1}{4}t^2 + \frac{1}{2}t + \frac{1}{4}) \sin(2t) + (\frac{3}{2}t + 2) \cos(2t) $$ This is the particular solution of the given second-order non-homogeneous linear differential equation. In an actual problem-solving situation using a computer algebra system, steps 4 to 6 would be performed by the program/framework you use, which would provide you with the coefficients A, B, C, D, E, and F directly.

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Key Concepts

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

Second-order Linear Differential Equation
Second-order linear differential equations are pivotal in understanding many physical phenomena, such as oscillation and wave behavior. They involve the second derivative of a function, which makes these equations crucial for modeling systems where acceleration or curvature needs to be described. These equations generally take the standard form: \(a(t)y'' + b(t)y' + c(t)y = g(t)\).
The left-hand side (LHS) of the equation includes terms like the second derivative \(y''\), a term for the first derivative \(y'\), and a term for the original function \(y\). The LHS is sometimes referred to as the homogeneous part of the equation when set to zero.
In the specific problem from the exercise, the differential equation is \(y'' + 4y = t^2 \sin 2t + (6t + 7) \cos 2t\).
Here, \(a(t) = 1\), \(b(t) = 0\), and \(c(t) = 4\), with \(g(t) = t^2 \sin 2t + (6t+7) \cos 2t\), providing the non-homogeneous part. Understanding this allows us to approach solutions using various methods applicable to second-order linear equations.
Non-homogeneous Differential Equation
A non-homogeneous differential equation contains a non-zero term on the right-hand side. This term, usually denoted as \(g(t)\), makes the equation more challenging to solve directly compared to its homogeneous counterpart. Non-homogeneous equations are significant because they allow us to describe systems influenced by external forces or inputs.
The typical structure of a non-homogeneous equation is \(a(t)y'' + b(t)y' + c(t)y = g(t)\), where \(g(t)\) often represents a function that could be a simple polynomial, trigonometric function, exponential, or a combination of these, as seen in the exercise problem.
To solve such equations, we often first find the complementary or homogeneous solution by setting \(g(t) = 0\). Then, we determine the particular solution that directly incorporates the structure of \(g(t)\). Combining both the complementary solution and the particular solution gives the complete response of the system.
Particular Solution
The particular solution is a crucial component used to solve non-homogeneous differential equations. This solution specifically addresses the non-homogeneous part \(g(t)\) of the equation, providing a way to incorporate its influence.
For the exercise's specific equation, \(y'' + 4y = t^2 \sin 2t + (6t+7) \cos 2t\), the particular solution needs to match the form of \(g(t)\). By implementing the method of undetermined coefficients, we propose a form like \(Y(t) = (A t^2 + B t + C) \sin(2t) + (D t^2 + E t + F) \cos(2t)\).
This form mirrors the trigonometric and polynomial nature of \(g(t)\). By substituting this assumed solution form back into the differential equation, you can solve for the unknown coefficients. This is where the method gets its name, as the coefficients are "undetermined" until solved using the equation.
The calculated particular solution for our problem integrates seamlessly with the complementary solution to offer a complete description of the system's behavior.
Computer Algebra System
Computer algebra systems (CAS) are powerful tools for solving complex mathematical problems, including differential equations. These systems can perform symbolic manipulations that automate solving, differentiating, and integrating functions.
Using a CAS, especially for problems involving the method of undetermined coefficients, can significantly simplify the process. Instead of manually calculating derivatives, substituting terms, and solving equations, a CAS handles these steps efficiently and accurately.
In our particular exercise, a CAS can be used to find the particular solution quickly by executing the mathematical steps involved in steps 4 to 6. With the CAS inputting the assumed particular form, extracting derivatives, substituting them into the differential equation, and solving for unknown coefficients become way more efficient. Ultimately, this advantage aids students and professionals alike to focus on understanding the underlying problem rather than cumbersome computations.

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Most popular questions from this chapter

Verify that the given functions \(y_{1}\) and \(y_{2}\) satisfy the corresponding homogeneous equation; then find a particular solution of the given nonhomogeneous equation. In Problems 19 and \(20 g\) is an arbitrary continuous function. $$ t y^{\prime \prime}-(1+t) y^{\prime}+y=t^{2} e^{2 i}, \quad t>0 ; \quad y_{1}(t)=1+t, \quad y_{2}(t)=e^{t} $$

A mass of \(20 \mathrm{g}\) stretches a spring \(5 \mathrm{cm}\). Suppose that the mass is also attached to a viscous damper with a damping constant of \(400 \mathrm{dyne}\) -sec/cm. If the mass is pulled down an additional \(2 \mathrm{cm}\) and then released, find its position \(u\) at any time \(t .\) Plot \(u\) versus \(t .\) Determine the quasi frequency and the quasi period. Determine the ratio of the quasi period to the period of the corresponding undamped motion. Also find the time \(\tau\) such that \(|u(t)|<0.05\) \(\mathrm{cm}\) for all \(t>\tau\)

Consider a vibrating system described by the initial value problem $$ u^{\prime \prime}+\frac{1}{4} u^{\prime}+2 u=2 \cos \omega t, \quad u(0)=0, \quad u^{\prime}(0)=2 $$ (a) Determine the steady-state part of the solution of this problem. (b) Find the amplitude \(A\) of the steady-state solution in terms of \(\omega\). (c) Plot \(A\) versus \(\omega\). (d) Find the maximum value of \(A\) and the frequency \(\omega\) for which it occurs.

Use the method of reduction of order to find a second solution of the given differential equation. \((x-1) y^{\prime \prime}-x y^{\prime}+y=0, \quad x>1 ; \quad y_{1}(x)=e^{x}\)

A series circuit has a capacitor of \(10^{-5}\) farad, a resistor of \(3 \times 10^{2}\) ohms, and an inductor of 0.2 henry. The initial charge on the capacitor is \(10^{-6}\) coulomb and there is no initial current. Find the charge \(Q\) on the capacitor at any time \(t .\)

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