Chapter 7: Problem 13
13\. Find the Laplace transform of \(f(t) :=\int^{t}(t-v) e^{3 v} d v\).
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Chapter 7: Problem 13
13\. Find the Laplace transform of \(f(t) :=\int^{t}(t-v) e^{3 v} d v\).
These are the key concepts you need to understand to accurately answer the question.
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The current \(I(t)\) in an \(L C\) series circuit is governed by the initial value problem $$I^{\prime \prime}(t)+4 I(t)=g(t)$$ $$I(0)=1, \quad I^{\prime}(0)=3$$ where $$g(t) : \left\\{\begin{array}{ll}{3 \sin t,} & {0 \leq t \leq 2 \pi} \\ {0,} & {2 \pi< t}\end{array}\right.$$ Determine the current as a function of time \(t .\)
Formally using integration by parts, show that $$\int_{-\infty}^{\infty} f(t) \delta^{\prime}(t) d t=-f^{\prime}(0)$$ Also show that, in general, $$\int_{-\infty}^{\infty} f(t) \delta^{(n)}(t) d t=(-1)^{n} f^{(n)}(0)$$
\(y^{\prime \prime}+y=3 \sin 2 t-3(\sin 2 t) u(t-2 \pi)\) \(y(0)=1, \quad y^{\prime}(0)=-2\)
\(\int_{-\infty}^{\infty}(\sin 3 t) \delta\left(t-\frac{\pi}{2}\right) d t\)
Figure 7.29 shows a beam of length 2\(\lambda\) that is imbed- ded in a support on the left side and free on the right. The vertical deflection of the beam a distance \(x\) from the support is denoted by \(y(x) .\) If the beam has a concen- trated load L acting on it in the center of the beam, then the deflection must satisfy the symbolic boundary value problem $$E I y^{(4)}(x)=L \delta(x-\lambda)$$ $$y(0)=y^{\prime}(0)=y^{\prime \prime}(2 \lambda)=y^{\prime \prime \prime}(2 \lambda)=0$$ where \(E,\) the modulus of elasticity, and \(I,\) the moment of inertia, are constants. Find a formula for the dis- placement \(y(x)\) in terms of the constants \(\lambda, L, E,\) and I. [Hint: Let \(y^{\prime \prime}(0)=A\) and \(y^{\prime \prime \prime}(0)=B .\) First solve the fourth-order symbolic initial value problem and then use the conditions \(y^{\prime \prime}(2 \lambda)=y^{\prime \prime \prime}(2 \lambda)=0\) to determine \(A\) and \(B . ]\)
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