Chapter 3: Problem 42
$$ \left(1+t^{2}\right) y^{\prime \prime}+2 t y^{\prime}+3 t^{-2}=0, \quad y(1)=2, \quad y^{\prime}(1)=-1 $$
Chapter 3: Problem 42
$$ \left(1+t^{2}\right) y^{\prime \prime}+2 t y^{\prime}+3 t^{-2}=0, \quad y(1)=2, \quad y^{\prime}(1)=-1 $$
All the tools & learning materials you need for study success - in one app.
Get started for freetry to transform the given equation into one with constant coefficients by the
method of Problem 34. If this is possible, find the general solution of the
given equation.
$$
t y^{\prime \prime}+\left(t^{2}-1\right) y^{\prime}+t^{3} y=0, \quad
0
A mass of \(20 \mathrm{g}\) stretches a spring \(5 \mathrm{cm}\). Suppose that the mass is also attached to a viscous damper with a damping constant of \(400 \mathrm{dyne}\) -sec/cm. If the mass is pulled down an additional \(2 \mathrm{cm}\) and then released, find its position \(u\) at any time \(t .\) Plot \(u\) versus \(t .\) Determine the quasi frequency and the quasi period. Determine the ratio of the quasi period to the period of the corresponding undamped motion. Also find the time \(\tau\) such that \(|u(t)|<0.05\) \(\mathrm{cm}\) for all \(t>\tau\)
Find the solution of the given initial value problem. $$ y^{\prime \prime}+4 y=t^{2}+3 e^{\prime}, \quad y(0)=0, \quad y^{\prime}(0)=2 $$
A spring-mass system has a spring constant of \(3 \mathrm{N} / \mathrm{m}\). A mass of \(2 \mathrm{kg}\) is attached to the spring and the motion takes place in a viscous fluid that offers a resistance numerically equal to the magnitude of the instantaneous velocity. If the system is driven by an external force of \(3 \cos 3 t-2 \sin 3 t \mathrm{N},\) determine the steady-state response. Express your answer in the form \(R \cos (\omega t-\delta)\)
By choosing the lower limitofation in Eq. ( 28 ) inthe textas the initial point \(t_{0}\), show that \(Y(t)\) becomes $$ Y(t)=\int_{t_{0}}^{t} \frac{y_{1}(s) y_{2}(t)-y_{1}(s) y_{2}(s)}{y_{1}(s) y_{2}^{2}(s)-y_{1}^{\prime}(s) y_{2}(s)} g(s) d s $$ Show that \(Y(t)\) is asolution of the initial value problem $$ L[y], \quad y\left(t_{0}\right)=0, \quad y^{\prime}\left(t_{0}\right)=0 $$ Thus \(Y\) can be identific d writh \(v\) in Problem \(21 .\)
What do you think about this solution?
We value your feedback to improve our textbook solutions.