Math Problem Statement

solve using laplace transform method y 00 − 2y 0 + y = δ(t − 1) y(0) = 3, y0 (0) = −4.

Solution

We aim to solve the differential equation

y2y+y=δ(t1),y(0)=3,y(0)=4y'' - 2y' + y = \delta(t - 1), \quad y(0) = 3, \quad y'(0) = -4

using the Laplace transform method.


Steps:

  1. Take the Laplace transform of the entire equation: Recall the Laplace transform rules:

    • L[y(t)]=s2Y(s)sy(0)y(0)\mathcal{L}[y''(t)] = s^2 Y(s) - sy(0) - y'(0)
    • L[y(t)]=sY(s)y(0)\mathcal{L}[y'(t)] = s Y(s) - y(0)
    • L[y(t)]=Y(s)\mathcal{L}[y(t)] = Y(s)
    • L[δ(ta)]=eas\mathcal{L}[\delta(t - a)] = e^{-as}

    Applying the Laplace transform to both sides of the equation: [ \mathcal{L}[y'' - 2y' + y] = \mathcal{L}[\delta(t - 1)] ]

    Using the initial conditions y(0)=3y(0) = 3 and y(0)=4y'(0) = -4: (s2Y(s)3s+4)2(sY(s)3)+Y(s)=es.(s^2 Y(s) - 3s + 4) - 2(s Y(s) - 3) + Y(s) = e^{-s}.

  2. Simplify the equation: Expand and group terms involving Y(s)Y(s): s2Y(s)3s+42sY(s)+6+Y(s)=es.s^2 Y(s) - 3s + 4 - 2s Y(s) + 6 + Y(s) = e^{-s}.

    Combine like terms: (s22s+1)Y(s)=es+3s10.(s^2 - 2s + 1) Y(s) = e^{-s} + 3s - 10.

    Simplify further: (s1)2Y(s)=es+3s10.(s - 1)^2 Y(s) = e^{-s} + 3s - 10.

    Solve for Y(s)Y(s): Y(s)=es+3s10(s1)2.Y(s) = \frac{e^{-s} + 3s - 10}{(s - 1)^2}.

  3. Perform partial fraction decomposition: Decompose 3s10(s1)2\frac{3s - 10}{(s - 1)^2}: 3s10(s1)2=As1+B(s1)2.\frac{3s - 10}{(s - 1)^2} = \frac{A}{s - 1} + \frac{B}{(s - 1)^2}.

    Solve for AA and BB by multiplying through by (s1)2(s - 1)^2: 3s10=A(s1)+B.3s - 10 = A(s - 1) + B.

    Expand and equate coefficients: 3s10=AsA+B.3s - 10 = As - A + B.

    Comparing coefficients of ss and constant terms:

    • Coefficient of ss: A=3A = 3,
    • Constant term: A+B=10-A + B = -10, so 3+B=10-3 + B = -10, giving B=7B = -7.

    Thus: 3s10(s1)2=3s17(s1)2.\frac{3s - 10}{(s - 1)^2} = \frac{3}{s - 1} - \frac{7}{(s - 1)^2}.

    Substitute back into Y(s)Y(s): Y(s)=es(s1)2+3s17(s1)2.Y(s) = \frac{e^{-s}}{(s - 1)^2} + \frac{3}{s - 1} - \frac{7}{(s - 1)^2}.

  4. Take the inverse Laplace transform: Break Y(s)Y(s) into parts and find the inverse Laplace transform:

    • L1[3s1]=3et\mathcal{L}^{-1}\left[\frac{3}{s - 1}\right] = 3e^t,
    • L1[7(s1)2]=7tet\mathcal{L}^{-1}\left[\frac{-7}{(s - 1)^2}\right] = -7te^t,
    • L1[es(s1)2]=u1(t)(t1)et1\mathcal{L}^{-1}\left[\frac{e^{-s}}{(s - 1)^2}\right] = u_1(t)(t - 1)e^{t - 1} (where u1(t)u_1(t) is the Heaviside function).

    Combine the terms: y(t)=3et7tet+u1(t)(t1)et1.y(t) = 3e^t - 7te^t + u_1(t)(t - 1)e^{t - 1}.


Final Solution:

y(t)=3et7tet+u1(t)(t1)et1.y(t) = 3e^t - 7te^t + u_1(t)(t - 1)e^{t - 1}.


Let me know if you need any steps clarified or further assistance! Here are related questions to deepen understanding:

  1. What is the role of the Heaviside function in solutions involving impulses like δ(t1)\delta(t - 1)?
  2. How does the Laplace transform simplify solving initial value problems?
  3. Why is partial fraction decomposition important in this context?
  4. What are the practical applications of impulse response in real-world systems?
  5. How can we verify the solution using an alternative method like direct integration?

Tip: Always remember to correctly incorporate initial conditions when applying the Laplace transform, as they are critical in shaping the solution.

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Math Problem Analysis

Mathematical Concepts

Differential Equations
Laplace Transform
Partial Fraction Decomposition
Impulse Response

Formulas

Laplace Transform: \( \mathcal{L}[y'(t)] = s Y(s) - y(0) \), \( \mathcal{L}[y''(t)] = s^2 Y(s) - s y(0) - y'(0) \)
Laplace Transform of Delta Function: \( \mathcal{L}[\delta(t - a)] = e^{-as} \)
Inverse Laplace Transform

Theorems

Properties of Laplace Transform
Linearity of Laplace Transform
Convolution Theorem

Suitable Grade Level

Grades 11-12, College Level