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Find the inverse Laplace transform of the given function. $$ \frac{3}{s^{2}+4} $$

Short Answer

Expert verified
Answer: The inverse Laplace transform of the given function is \(f(t) = 3\sin(2t)\).

Step by step solution

01

Identify a Laplace Transform Pair

From the Laplace transform table, we can find a pair of the form: $$ \mathcal{L}\{f(t)\} = \frac{k}{s^{2} + k^2} $$ Where the inverse Laplace transform can be determined as: $$ f(t) = \mathcal{L}^{-1}\{\frac{k}{s^{2} + k^2}\} = k\sin(kt) $$
02

Match the Given Function with the Laplace Transform Pair

For our given function, we have: $$ \frac{3}{s^{2}+4} $$ By comparing this function with the standard Laplace transform pair, we can identify the constants as: $$ k = \sqrt{4}=2 $$ This means that our function f(t) is scaled by a factor of 3/2.
03

Determine the Inverse Laplace Transform

Now, we can find the inverse Laplace transform of our given function, using the known inverse Laplace transform of the identified pair: $$ f(t) = \mathcal{L}^{-1}\{\frac{3}{s^{2}+4}\} = \frac{3}{2} (2\sin(2t)) $$ Simplifying the expression: $$ f(t) = 3\sin(2t) $$ The inverse Laplace transform of the given function \(\frac{3}{s^{2}+4}\) is \(f(t) = 3\sin(2t)\).

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Key Concepts

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

Laplace Transform Pairs
Understanding Laplace Transform Pairs is essential when finding the inverse Laplace transform of a function. Laplace transform pairs consist of a function in the time domain and its corresponding representation in the Laplace domain. For example, the function \( f(t) = k\sin(kt) \) in the time domain corresponds to \( \frac{k}{s^2 + k^2} \) in the Laplace domain.
This relationship allows us to easily switch between the time and Laplace domains using transformation tables, which list common pairs. By identifying these pairs, we can solve differential equations and analyze systems that are described by these equations.
  • Transforms are used to convert differential equations into algebraic equations, which are easier to manipulate.
  • Laplace tables help find these transforms quickly and efficiently.
Recognizing these pairs is crucial for engineers and scientists in applications involving control systems and signal processing.
Sine Function
The sine function is a fundamental concept when dealing with waveforms and oscillations. In the context of Laplace transforms, the sine function is often part of the solution for systems experiencing periodic behavior. Specifically, the Laplace transform of a sine function \( \sin(kt) \) is \( \frac{k}{s^2 + k^2} \).
Sine functions represent smooth repetitive oscillations that can describe various physical phenomena, including sound waves and alternating current.
  • The amplitude of the sine function determines the peak value of the wave.
  • The frequency of the sine function, given by \( k \), determines how fast the oscillation occurs.
Understanding the interplay between the Laplace domain and the time domain representations allows us to accurately capture and solve problems related to waves and oscillations.
Solving Differential Equations
Solving differential equations using Laplace transforms involves transforming the problem into a more manageable algebraic form. This powerful method is especially handy when dealing with linear differential equations with constant coefficients. Once transformed, these equations can be solved more straightforwardly.
The main steps in this process include:
  • Applying the Laplace transform to each term in the differential equation.
  • Rewriting the initial conditions in the Laplace domain if given.
  • Solving the resulting algebraic equation.
  • Converting the solution back to the time domain using the inverse Laplace transform.
This technique simplifies the process of solving complex differential equations, making it a favored choice among engineers and mathematicians working with dynamic systems and signals.

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Most popular questions from this chapter

Concerned with differentiation of the Laplace transform. Let $$ F(s)=\int_{0}^{\infty} e^{-s i} f(t) d t $$ It is possible to show that as long as \(f\) satisfics the conditions of Theorem \(6.1 .2,\) it is legitimate to differentiate under the integral sign with respect to the parameter \(s\) when \(s>a .\) (a) Show that \(F^{\prime}(s)=\mathcal{L}\\{-l f(t)\\}\) (b) Show that \(F^{(n)}(s)=\mathcal{L}\left\\{(-t)^{n} f(t)\right\\} ;\) hence differentiating the Laplace transform corresponds to multiplying the original function by \(-t .\)

Recall that cos bt \(=\left(e^{i b t}+e^{t b t}\right) / 2\) and \(\sin b t=\left(e^{j b t}-\right.\) \(\left.e^{-t b t}\right) / 2 i .\) Assuming that the necessary elementary integration formulas extend to this case, find the Laplace transform of the given function; \(a\) and \(b\) are real constants. $$ e^{a t} \cos b t $$

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

Express the solution of the given initial value problem in terms of a convolution integral. \(y^{\prime \prime}+3 y^{\prime}+2 y=\cos \alpha t ; \quad y(0)=1, \quad y^{\prime}(0)=0\)

The Laplace transforms of certain functions can be found conveniently from their Taylor series expansions. (a) Using the Taylor series for \(\sin t\) $$ \sin t=\sum_{n=0}^{\infty} \frac{(-1)^{n} t^{2 n+1}}{(2 n+1) !} $$ and assuming that the Laplace transform of this scries can be computed term by term, verify that $$ \mathcal{L}\\{f(t)\\}=\arctan (1 / s), \quad s>1 $$ (c) The Bessel function of the first kind of order zero \(J_{0}\) has the Taylor series (see Section 5.8 ) $$ J_{0}(t)=\sum_{n=0}^{\infty} \frac{(-1)^{n} t^{2 n}}{2^{2 n}(n !)^{2}} $$ Assuming that the following Laplace transforms can be computed term by term, verify that $$ \mathcal{L}\left\\{J_{0}(t)\right\\}=\left(s^{2}+1\right)^{-1 / 2}, \quad s>1 $$ and $$\mathcal{L}\left[J_{0}(\sqrt{t})\right\\}=s^{-1} e^{-1 / 4 s}, \quad s>0$$

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