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Find the inverse Laplace transform of the given function. $$ \frac{2 s-3}{s^{2}+2 s+10} $$

Short Answer

Expert verified
Answer: The inverse Laplace transform of the function \( \frac{2 s-3}{s^{2}+2 s+10} \) is \( f(t) = 2e^{-t}\cos(3t) - \frac{5}{3}e^{-t}\sin(3t) \).

Step by step solution

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01

Identify the form of the given function

The given function can be written as a combination of standard Laplace transforms. To do that, we need to use partial fraction decomposition and rewrite the given function in the form of a sum of simpler fractions.
02

Partial fraction decomposition

We'll first complete the square in the denominator, and then perform partial fraction decomposition: $$ \frac{2s-3}{s^{2}+2 s+10} = \frac{2s - 3}{(s + 1)^{2} + 3^{2}} $$ Now we rewrite the given function in the form of a sum of simpler fractions: $$ \frac{2s - 3}{(s + 1)^{2} + 3^{2}} = \frac{A(s + 1) + B}{(s + 1)^{2} + 3^{2}} $$ Equating the numerators, we have: $$ 2s - 3 = A(s + 1) + B $$ By comparing coefficients, we get: \(A = 2\), and \(B = -5\) So, the given function can be written as: $$ \frac{2s - 3}{(s + 1)^{2} + 3^{2}} = \frac{2(s + 1) - 5}{(s + 1)^{2} + 3^{2}} $$
03

Inverse Laplace Transform

Now, we can identify the standard Laplace transform and find its inverse using inverse Laplace transform formulas: The inverse Laplace transform of a given function is given by: $$ \mathcal{L}^{-1}\left\{\frac{2s - 3}{(s + 1)^{2} + 3^{2}}\right\} = \mathcal{L}^{-1}\left\{\frac{2(s + 1) - 5}{(s + 1)^{2} + 3^{2}}\right\} $$ Inverse Laplace transform of a standard function in the form \(\frac{s - a}{(s - a)^{2} + b^{2}}\) is given by: $$ \mathcal{L}^{-1}\left\{\frac{s-a}{(s-a)^{2} + b^{2}}\right\} = e^{at}\cos(bt) $$ and the inverse Laplace transform of a standard function in the form \(\frac{1}{(s - a)^{2} + b^{2}}\) is given by: $$ \mathcal{L}^{-1}\left\{\frac{1}{(s - a)^{2} + b^{2}}\right\} = e^{at}\frac{\sin(bt)}{b} $$ Using the above formulas, we get: $$ \mathcal{L}^{-1}\left\{\frac{2(s + 1) - 5}{(s + 1)^{2} + 3^{2}}\right\} = \mathcal{L}^{-1}\left\{2\frac{(s + 1)}{(s + 1)^{2} + 3^{2}}\right\} - \mathcal{L}^{-1}\left\{5\frac{1}{(s + 1)^{2} + 3^{2}}\right\} $$ $$ = 2e^{-t}\cos(3t) - 5e^{-t}\frac{\sin(3t)}{3} $$ So, the inverse Laplace transform of the given function is: $$ f(t) = 2e^{-t}\cos(3t) - \frac{5}{3}e^{-t}\sin(3t) $$

Key Concepts

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

partial fraction decomposition
Partial fraction decomposition is a method used to break down complex rational expressions into simpler fractions. This technique is valuable for finding inverse Laplace transforms, as it simplifies the process of matching terms with known Laplace transform pairs.
In the given exercise, we started with the fraction \( \frac{2s - 3}{s^{2} + 2s + 10} \). To facilitate decomposition, we first completed the square on the denominator, rewriting it as \((s + 1)^{2} + 3^{2}\).
Then, we represented the numerator as a linear combination aligned with the denominator, \( A(s + 1) + B \). Solving for \( A \) and \( B \) by comparing coefficients gave us simple terms that are easier to invert using known Laplace transform formulas.
standard Laplace transforms
Standard Laplace transforms are fundamental transformations used to convert time-domain functions into the complex frequency domain, where they are easier to manipulate and solve.
The inverse of these standard transforms allows us to revert back to the time domain. In solving the exercise, the function was rewritten using standard forms with \( s \) shifted by "+1" due to the completed square in the denominator.
This manipulation is crucial since it aligns the problem with standard inverse Laplace transform formulas, allowing a straightforward calculation. Remember, this typically involves either cosine or sine formulas.
inverse Laplace transform formulas
Inverse Laplace transform formulas are essential for translating functions from the complex frequency domain back to the time domain. These formulas match complex expressions to time-domain functions, such as exponentials and trigonometric functions.
For the exercise function \( \frac{2s - 3}{(s + 1)^{2} + 3^{2}} \), we used the following inverse formulas:
  • \( \mathcal{L}^{-1}\{ \frac{s-a}{(s-a)^{2} + b^{2}} \} = e^{at}\cos(bt) \)
  • \( \mathcal{L}^{-1}\{ \frac{1}{(s-a)^{2} + b^{2}} \} = e^{at}\frac{\sin(bt)}{b} \)
These formulas relate the time shift and the oscillating behavior (either cosine or sine) based on shifts in the complex frequency "s".
They were applied directly to the terms of the partial fraction decomposition, resulting in a combination of exponential decay, cosine, and sine terms.
cosine and sine transforms
Cosine and sine transforms form the backbone of inverse Laplace transforms for harmonic oscillators in engineering and physics. They describe oscillatory behaviors seen in mechanical and electrical systems.
In the exercise, the inverse transform involved two main components: an exponential decay function multiplied by either the cosine or sine functions.
  • The formula \( e^{at}\cos(bt) \) corresponds to the inverse Laplace transform of shifting along \( s \) and relates to damped cosine oscillations.
  • The formula \( e^{at}\frac{\sin(bt)}{b} \) deals with similar sine oscillations.
These components combined to describe the overall time-domain behavior of the original complex expression, denoted by \( f(t) = 2e^{-t}\cos(3t) - \frac{5}{3}e^{-t}\sin(3t) \). Thus, by utilizing cosine and sine transforms, we can represent how a system evolves over time with oscillatory decay.

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Most popular questions from this chapter

Recall that \(\cosh b t=\left(e^{b t}+e^{-b t}\right) / 2\) and \(\sinh b t=\left(e^{b t}-e^{-b t}\right) / 2 .\) In each of Problems 7 through 10 find the Laplace transform of the given function; \(a\) and \(b\) are real constants. $$ \cosh b t $$

Express the solution of the given initial value problem in terms of a convolution integral. \(4 y^{\prime \prime}+4 y^{\prime}+17 y=g(t) ; \quad y(0)=0, \quad y^{\prime}(0)=0\)

Use the Laplace transform to solve the given initial value problem. $$ y^{\mathrm{iv}}-4 y=0 ; \quad y(0)=1, \quad y^{\prime}(0)=0, \quad y^{\prime \prime}(0)=-2, \quad y^{\prime \prime \prime}(0)=0 $$

Find the inverse Laplace transform of the given function. $$ F(s)=\frac{e^{-2 s}}{s^{2}+s-2} $$

The Tautochrone. A problem of interest in the history of mathematics is that of finding the tautochrone-the curve down which a particle will slide freely under gravity alone, reaching the bottom in the same time regardless of its starting point on the curve. This problem arose in the construction of a clock pendulum whose period is independent of the amplitude of its motion. The tautochrone was found by Christian Huygens \((1629-\) \(1695)\) in 1673 by geometrical methods, and later by Leibniz and Jakob Bernoulli using analytical arguments. Bernoulli's solution (in \(1690)\) was one of the first occasions on which a differential equation was explicitly solved. The Tautochrone. A problem of interest in the history of mathematics is that of finding the tautochrone-the curve down which a particle will slide freely under gravity alone, reaching the bottom in the same time regardless of its starting point on the curve. This problem arose in the construction of a clock pendulum whose period is independent of the amplitude of its motion. The tautochrone was found by Christian Huygens \((1629-\) \(1695)\) in 1673 by geometrical methods, and later by Leibniz and Jakob Bernoulli using analytical arguments. Bernoulli's solution (in \(1690)\) was one of the first occasions on which a differential equation was explicitly solved. The geometrical configuration is shown in Figure \(6.6 .2 .\) The starting point \(P(a, b)\) is joined to the terminal point \((0,0)\) by the arc \(C .\) Arc length \(s\) is measured from the origin, and \(f(y)\) denotes the rate of change of \(s\) with respect to \(y:\) $$ f(y)=\frac{d s}{d y}=\left[1+\left(\frac{d x}{d y}\right)^{2}\right]^{1 / 2} $$ Then it follows from the principle of conservation of energy that the time \(T(b)\) required for a particle to slide from \(P\) to the origin is $$ T(b)=\frac{1}{\sqrt{2 g}} \int_{0}^{b} \frac{f(y)}{\sqrt{b-y}} d y $$

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