Chapter 6: Problem 5
Find the inverse Laplace transform of the given function. $$ \frac{2 s+2}{s^{2}+2 s+5} $$
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Chapter 6: Problem 5
Find the inverse Laplace transform of the given function. $$ \frac{2 s+2}{s^{2}+2 s+5} $$
These are the key concepts you need to understand to accurately answer the question.
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Get started for freeUse the result of Problem 28 to find the Laplace transform of the given function; \(a\) and \(b\) are real numbers and \(n\) is a positive integer. $$ t e^{a t} \cos b t $$
Find the inverse Laplace transform of the given function. $$ \frac{2 s-3}{s^{2}-4} $$
Use the Laplace transform to solve the given initial value problem. $$ y^{\prime \prime}-2 y^{\prime}+2 y=e^{-t} ; \quad y(0)=0, \quad y^{\prime}(0)=1 $$
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 $$ T(b)=\frac{1}{\sqrt{2 g}} \int_{0}^{b} \frac{f(y)}{\sqrt{b-y}} d y $$
Find the inverse Laplace transform of the given function. $$ \frac{3}{s^{2}+4} $$
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