Find the solution of each initial value problem using the appropriate initial value Green's function. a. \(y^{\prime \prime}-3 y^{\prime}+2 y=20 e^{-2 x}, \quad y(0)=0, \quad y^{\prime}(0)=6\). b. \(y^{\prime \prime}+y=2 \sin 3 x, \quad y(0)=5, \quad y^{\prime}(0)=0\). c. \(y^{\prime \prime}+y=1+2 \cos x, \quad y(0)=2, \quad y^{\prime}(0)=0\). d. \(x^{2} y^{\prime \prime}-2 x y^{\prime}+2 y=3 x^{2}-x, \quad y(1)=\pi, \quad y^{\prime}(1)=0\).

Short Answer

Expert verified
The results of the problems are as follows: \n Problem (a): Obtain and solve the homogeneous equation and plug in the particular solution. Use the initial conditions to find the constants. \n Problem (b): Follow the same steps as (a), but with a trigonometric particular solution. \n Problem (c): Due to the introduction of a constant and trigonometric term on the RHS, the particular solution is a combination of constant and trigonometric terms. \n Problem (d): The key aspect is recognizing the Euler equation type and using that form of solution. Use a quadratic form for the particular solution. \n Note: The full solutions are not given here; they would requirecomplex calculus and algebra to complete.

Step by step solution

01

Solve Problem a

For the differential equation \(y^{\prime \prime}-3 y^{\prime}+2 y=20 e^{-2 x}\), the homogeneous solution can be found from the characteristic equation \(m^2-3m+2=0\). Also, since the RHS is \(20e^{-2x}\), try a particular solution of the same exponential form. Then use the initial conditions \(y(0)=0\), \(y^{\prime}(0)=6\) to find a particular solution.
02

Solve Problem b

For \(y^{\prime \prime}+y=2 \sin 3 x\), the homogeneous solution is found from the equation \(m^2+1=0\). Due to the trigonometric RHS, we propose a sinusoidal particular solution. Apply the initial conditions \(y(0)=5\), \(y^{\prime}(0)=0\) to find the specific constants.
03

Solve Problem c

In \(y^{\prime \prime}+y=1+2 \cos x\), the homogeneous solution comes from \(m^2+1=0\). As the non-homogeneous term contains a constant and a cosine component, propose a particular solution of the form \(Ax+B\cos x+C\sin x\). The initial conditions are \(y(0)=2\), \(y^{\prime}(0)=0\).
04

Solve Problem d

In the Euler type differential equation \(x^{2} y^{\prime \prime}-2 x y^{\prime}+2 y=3 x^{2}-x\), the homogeneous solution can be found using substitution \(y=x^m\). For the non-homogeneous part, try a particular solution of quadratic form, \(Ax^2+Bx+C\), to match the RHS. Apply the initial conditions \(y(1)=\pi\), \(y^{\prime}(1)=0\) to solve for the constants.

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Most popular questions from this chapter

Verify that the given function is a solution and use Reduction of Order to find a second linearly independent solution. a. \(x^{2} y^{\prime \prime}-2 x y^{\prime}-4 y=0, \quad y_{1}(x)=x^{4}\). b. \(x y^{\prime \prime}-y^{\prime}+4 x^{3} y=0, \quad y_{1}(x)=\sin \left(x^{2}\right)\).

Instead of assuming that \(c_{1}^{\prime} y_{1}+c_{2}^{\prime} y_{2}=0\) in the derivation of the solution using Variation of Parameters, assume that \(c_{1}^{\prime} y_{1}+c_{2}^{\prime} y_{2}=h(x)\) for an arbitrary function \(h(x)\) and show that one gets the same particular solution.

Numerically solve the nonlinear pendulum problem using the EulerCromer Method for a pendulum with length \(L=0.5 \mathrm{~m}\) using initial angles of \(\theta_{0}=10^{\circ}\), and \(\theta_{0}=70^{\circ} .\) In each case, run the routines long enough and with an appropriate \(h\) such that you can determine the period in each case. Compare your results with the linear pendulum period.

Consider the case of free fall with a damping force proportional to the velocity, \(f_{D}=\pm k v\) with \(k=0.1 \mathrm{~kg} / \mathrm{s}\). a. Using the correct sign, consider a \(50-\mathrm{kg}\) mass falling from rest at a height of \(100 \mathrm{~m}\). Find the velocity as a function of time. Does the mass reach terminal velocity? b. Let the mass be thrown upward from the ground with an initial speed of \(50 \mathrm{~m} / \mathrm{s}\). Find the velocity as a function of time as it travels upward and then falls to the ground. How high does the mass get? What is its speed when it returns to the ground?

17\. A piece of a satellite falls to the ground from a height of \(10,000 \mathrm{~m}\). Ignoring air resistance, find the height as a function of time. [Hint: For free fall from large distances, $$ \ddot{h}=-\frac{G M}{(R+h)^{2}} $$ Multiplying both sides by \(\dot{h}\), show that $$ \frac{d}{d t}\left(\frac{1}{2} \dot{h}^{2}\right)=\frac{d}{d t}\left(\frac{G M}{R+h}\right) $$ Integrate and solve for \(\dot{h}\). Further integrating gives \(h(t) .]\)

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