Chapter 4: Problem 19
$$4 y^{\prime \prime}+11 y^{\prime}-3 y=-2 t e^{-3 t}$$
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Chapter 4: Problem 19
$$4 y^{\prime \prime}+11 y^{\prime}-3 y=-2 t e^{-3 t}$$
These are the key concepts you need to understand to accurately answer the question.
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Prove the sum of angles formula for the sine function by following these steps. Fix x. (a) Let $$f(t) :=\sin (x+t)$$ Show that $$f^{\prime \prime}(t)+f(t)=0$$ $$f(0)=\sin x, \text { and } f^{\prime}(0)=\cos x$$ (b) Use the auxiliary equation technique to solve the initial value problem $$y^{\prime \prime}+y=0,y(0)=\sin x$$ and $$y^{\prime}(0)=\cos x$$ (c) By uniqueness, the solution in part (b) is the same as f1t2 from part (a). Write this equality; this should be the standard sum of angles formula for sin $$(x+t)$$
(True or False): If $$f_{1}, f_{2}, f_{3}$$ are three functions defined on $$(-\infty, \infty)$$ that are pairwise linearly independent on $$(-\infty, \infty)$$, then $$f_{1}, f_{2}, f_{3}$$ form a linearly independent set on $$(-\infty, \infty)$$. Justify your answer.
\(t(t-3) y^{\prime \prime}+2 t y^{\prime}-y=t^{2}\)
Wronskian. For any two differentiable functions \(y_{1}\) and \(y_{2}\), the function (18) $$\quad w\left[y_{1}, y_{2}\right](t)=y_{1}(t) y_{2}^{\prime}(t)-y_{1}^{\prime}(t) y_{2}(t$$ is called the Wronskian of $$y_{1}$$ and $$y_{2}$$. This function plays a crucial role in the proof of Theorem 2. (a) Show that $$W\left[y_{1}, y_{2}\right]$$ can be conveniently expressed as the $$2 \times 2$$ determinant $$W\left[y_{1}, y_{2}\right](t)=\left| \begin{array}{ll}{y_{1}(t)} & {y_{2}(t)} \\ {y_{1}^{\prime}(t)} & {y_{2}^{\prime}(t)}\end{array}\right|$$ (b) Let $$y_{1}(t), y_{2}(t)$$ be a pair of solutions to the homogeneous equation $$a y^{\prime \prime}+b y^{\prime}+c y=0$$ (with$$a \neq 0 )$$ on an open interval I. Prove that $$y_{1}(t)$$ and $$y_{2}(t)$$ are linearly independent on I if and only if their Wronskian is never zero on I. [Hint: This is just a reformulation of Lemma 1.] (c) Show that if $$y_{1}(t)$$ and $$y_{2}(t)$$ are any two differentiable functions that are linearly dependent on I, then their Wronskian is identically zero on I.
A vibrating spring without damping can be modeled by the initial value problem ( 11 ) in Example 3 by taking \(b=0\). (a) If \(m=10 \mathrm{~kg}, k=250 \mathrm{~kg} / \mathrm{sec}^{2}, y(0)=0.3 \mathrm{~m},\) and \(y^{\prime}(0)=-0.1 \mathrm{~m} / \mathrm{sec},\) find the equation of motion for this undamped vibrating spring. (b) After how many seconds will the mass in part (a) first cross the equilibrium point? (c) When the equation of motion is of the form displayed in (9), the motion is said to be oscillatory with frequency \(\beta / 2 \pi .\) Find the frequency of oscillation for the spring system of part (a).
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