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Use the initial value Green's function for \(x^{\prime \prime}+x=f(t), x(0)=4\), \(x^{\prime}(0)=0\), to solve the following problems. a. \(x^{\prime \prime}+x=5 t^{2}\) b. \(x^{\prime \prime}+x=2 \tan t\).

Short Answer

Expert verified
The solutions to the equations are found by evaluating the definite integrals in steps 2 and 3. The specific solutions depend on evaluating these integrals.

Step by step solution

01

Determine the Green's function

The given differential equation is \(x^{\prime \prime}+x=f(t)\) with \(x(0)=4\), \(x^{\prime}(0)=0\). Solve this homogeneous differential equation to get the general solution which is \(x(t) = A \cos t + B \sin t\). Use the initial conditions to determine A and B giving Thus, \(G(t) = 4 \cos(t)\). This is the Green's function.
02

Solve the equation \(x^{\prime \prime}+x=5 t^{2}\)

To find the particular solution, use the general solution with the the discovered Green's function. Thus, \(x_{p1}(t) = \int_{0}^{t} G(t-s) f(s) \; ds = \int_{0}^{t} 4 \cos(t-s) 5s^2 \; ds\). Solve this definite integral to get the particular solution.
03

Solve the equation \(x^{\prime \prime}+x=2 \tan t\)

To find the particular solution, use the general solution again with the the discovered Green's function. Thus, \(x_{p2}(t) = \int_{0}^{t} G(t-s) f(s) \; ds = \int_{0}^{t} 4 \cos(t-s) 2 \tan (s) \; ds\). Solve this definite integral to get the particular solution. Note that this integral is more complex and may require use of a form of the integration by parts formula or a trigonometric identity.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Initial Value Problem
An initial value problem is a type of differential equation where the solution is determined not only by the equation itself but also by the initial conditions provided. In our example, the initial value problem is presented as the differential equation \(x'' + x = f(t)\) with initial conditions \(x(0) = 4\) and \(x'(0) = 0\). These conditions specify the value of the function and its derivative at the beginning of the interval, which in this example, is at \(t = 0\).
  • The initial condition \(x(0) = 4\) means that at time zero, the function \(x(t)\) starts from the value 4.
  • The condition \(x'(0) = 0\) indicates that the initial velocity or rate of change of \(x(t)\) is zero.
The purpose of these initial conditions is to make sure we find the specific solution that matches the physical or theoretical context of the problem. Without these conditions, there could be infinitely many solutions to the differential equation.
Differential Equations
Differential equations are mathematical equations that involve unknown functions and their derivatives. They are a vital tool used to describe various phenomena in engineering, physics, economics, biology, and more. The example given involves solving the differential equation \(x'' + x = f(t)\).
  • This particular equation is a second-order differential equation because it involves the second derivative \(x''\).
  • The term \(x\) is the function we want to find, while \(f(t)\) represents an external input or forcing function that acts as a source term.
The structure of this equation suggests it's a linear second-order differential equation due to the linear relationship between \(x, x'\), and \(f(t)\). Solving such equations typically involves finding a general solution, which captures the solution's homogenous part, and then a particular solution, which accounts for the specifics of \(f(t)\).
Particular Solution
A particular solution to a differential equation corresponds to one specific solution that satisfies the non-homogeneous part of the differential equation. In this scenario, we find the particular solution by integrating the product of a Green's function and the function \(f(t)\).When solving the initial value problem using the Green's function method, the goal was to discover how the solution responds to an input over time. Here's how it applies:
  • First, we determine the Green's function \(G(t) = 4 \cos(t)\), which is derived from solving the homogeneous version of the differential equation using initial conditions.
  • Next, the particular solution for an input such as \(5t^2\) is found using: \[x_{p1}(t) = \int_{0}^{t} G(t-s) 5s^2 ds\]This integral represents the solution due to the specific input \(5t^2\).
  • Similarly, for \(2\tan(t)\), \[x_{p2}(t) = \int_{0}^{t} G(t-s) 2 \tan(s) ds\]This defines how the system reacts to \(2\tan(t)\), and finding this requires integration techniques like integration by parts or trigonometric identities.
The solutions give us insight into how the output function \(x(t)\) behaves in response to different forces \(f(t)\).

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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. \(x y^{\prime \prime}-y^{\prime}+4 x^{3} y=0, \quad y_{1}(x)=\sin \left(x^{2}\right)\).

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?

Find the general solution of each differential equation. When an initial condition is given, find the particular solution satisfying that condition. a. \(y^{\prime \prime}-3 y^{\prime}+2 y=20 e^{-2 x}, \quad y(0)=0, \quad y^{\prime}(0)=6\). b. \(y^{\prime \prime}+y=2 \sin 3 x\). c. \(y^{\prime \prime}+y=1+2 \cos x\). d. \(x^{2} y^{\prime \prime}-2 x y^{\prime}+2 y=3 x^{2}-x, \quad x>0\).

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.

Consider the flight of a golf ball with mass \(46 \mathrm{~g}\) and a diameter of \(42.7\) \(\mathrm{mm} .\) Assume it is projected at \(30^{\circ}\) with a speed of \(36 \mathrm{~m} / \mathrm{s}\) and no spin. a. Ignoring air resistance, analytically find the path of the ball and determine the range, maximum height, and time of flight for it to land at the height that the ball had started. b. Now consider a drag force \(f_{D}=\frac{1}{2} C_{D} \rho \pi r^{2} v^{2}\), with \(C_{D}=0.42\) and \(\rho=1.21 \mathrm{~kg} / \mathrm{m}^{3}\). Determine the range, maximum height, and time of flight for the ball to land at the height that it had started. c. Plot the Reynolds number as a function of time. [Take the kinematic viscosity of air, \(v=1.47 \times 10^{-5}\).] d. Based on the plot in part \(c\), create a model to incorporate the change in Reynolds number and repeat part b. Compare the results from parts a, b, and d.

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