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Find the Laplace transform of \(f(t)=\cos a t,\) where \(a\) is a real constant.

Short Answer

Expert verified
Answer: The Laplace transform of the function \(f(t) = \cos(at)\) is \(F(s) = \frac{s}{s^2+a^2}\).

Step by step solution

01

Identify the given function and the definition of Laplace transform

We are given the function \(f(t) = \cos{at}\) and tasked with finding its Laplace transform. The Laplace transform is defined as \(F(s) = \int_0^\infty e^{-st} f(t) dt\). So, we need to find the following integral: $$ F(s) = \int_0^\infty e^{-st} \cos{at} dt $$
02

Integration by Parts

To solve the above integral, we'll need to use integration by parts. Let $$ u = \cos{at};\, dv = e^{-st} dt $$ Now we find the derivative of \(u\) and the integral of \(dv\): $$ du = -a \sin{at} dt;\, v = -\frac{1}{s}e^{-st} $$ Using the formula for integration by parts, \(u \, dv = u \, v - \int v \, du\), we have: $$ \int e^{-st} \cos{at} dt = -\frac{1}{s}e^{-st}\cos{(at)} - \int -\frac{1}{s}e^{-st}(-a\sin{at}) dt $$ Simplifying the integral and rearranging terms, we get: $$ \int e^{-st} \cos{at} dt = -\frac{1}{s}e^{-st}\cos{(at)} + \frac{a}{s} \int e^{-st}\sin{at} dt $$
03

Apply Integration by Parts Again

We'll use integration by parts once more to resolve the remaining integral. This time let: $$ u = \sin{at};\, dv = e^{-st} dt $$ Calculate the derivative and integral again: $$ du = a\cos{(at)} dt;\, v = -\frac{1}{s}e^{-st} $$ Using the formula for integration by parts, \(u \, dv = u \, v - \int v \, du\), we have: $$ \int e^{-st} \sin{at} dt = -\frac{1}{s}e^{-st}\sin{at} - \int -\frac{1}{s}e^{-st}(a\cos{at}) dt $$ Now, simplifying and rearranging terms, we get: $$ \int e^{-st} \sin{at} dt = -\frac{1}{s}e^{-st}\sin{at} + \frac{a}{s^2} \int e^{-st}\cos{at} dt $$
04

Combine Results and Solve for \(F(s)\)

Now we have: $$ F(s) = -\frac{1}{s}e^{-st}\cos{(at)} + \frac{a}{s} \left(-\frac{1}{s}e^{-st}\sin{at} + \frac{a}{s^2} \int e^{-st}\cos{at} dt \right) $$ Note that the last integral term on the right is the original integral we wanted to solve for. We can rewrite the equation as: $$ F(s) - \frac{a^2}{s^3}F(s) = -\frac{1}{s}e^{-st}\cos{(at)} - \frac{a}{s^2}e^{-st}\sin{(at)} $$ Now, combine the terms with \(F(s)\): $$ \square (F(s)) = s^2 F(s) - a^2 F(s) = \int_0^\infty e^{-st} \cos{at} dt $$ The final step is to take the inverse Laplace transform
05

Evaluate the Result

Since we want to find the Laplace transform \(F(s)\) of the function \(f(t) = \cos{at}\), we have: $$ F(s) = \frac{s}{s^2+a^2}

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Most popular questions from this chapter

Find the inverse Laplace transform of the given function by using the convolution theorem. \(F(s)=\frac{G(s)}{s^{2}+1}\)

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 $$ T(b)=\frac{1}{\sqrt{2 g}} \int_{0}^{b} \frac{f(y)}{\sqrt{b-y}} d y $$

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 \(-t .\)

Find the inverse Laplace transform of the given function. $$ F(s)=\frac{2(s-1) e^{-2 s}}{s^{2}-2 s+2} $$

For each of the following initial value problems use the results of Problem 28 to find the differential equation satisfied by \(Y(s)=\mathcal{L}[\phi(t)\\},\) where \(y=\phi(t)\) is the solution of the given initial value problem. \(\begin{array}{ll}{\text { (a) } y^{\prime \prime}-t y=0 ;} & {y(0)=1, \quad y^{\prime}(0)=0 \text { (Airy's equation) }} \\ {\text { (b) }\left(1-t^{2}\right) y^{\prime \prime}-2 t y^{\prime}+\alpha(\alpha+1) y=0 ;} & {y(0)=0, \quad y^{\prime}(0)=1 \text { (Legendre's equation) }}\end{array}\) Note that the differential equation for \(Y(s)\) is of first order in part (a), but of second order in part (b). This is duc to the fact that \(t\) appcars at most to the first power in the equation of part (a), whereas it appears to the second power in that of part (b). This illustrates that the Laplace transform is not often useful in solving differential equations with variable coefficients, unless all the coefficients are at most linear functions of the independent variable.

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