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Assume, for the given differential equation, that \(y(0)=1\). (a) Use the differential equation itself to determine the values \(y^{\prime}(0), y^{\prime \prime}(0), y^{\prime \prime \prime}(0), y^{(4)}(0)\) and form the Taylor polynomial $$ P_{4}(t)=y(0)+y^{\prime}(0) t+\frac{y^{\prime \prime}(0)}{2 !} t^{2}+\frac{y^{\prime \prime \prime}(0)}{3 !} t^{3}+\frac{y^{(4)}(0)}{4 !} t^{4} $$ (b) Verify that the given function is the solution of the initial value problem consisting of the differential equation and initial condition \(y(0)=1\). (c) Evaluate both the exact solution \(y(t)\) and \(P_{4}(t)\) at \(t=0.1\). What is the error \(E(0.1)=y(0.1)-P_{4}(0.1)\) ? [Note that \(E(0.1)\) is the local truncation error incurred in using a Taylor series method of order 4 to step from \(t_{0}=0\) to \(t_{1}=0.1\) using step size \(h=0.1 .]\) \(y^{\prime}=y^{3 / 4} ; \quad y(t)=\left(1+\frac{t}{4}\right)^{4}\)

Short Answer

Expert verified
Answer: The error E(0.1) is approximately 0, indicating that the Taylor polynomial accurately approximates the function at t=0.1.

Step by step solution

01

Find the given differential equation and initial value at t=0

The given differential equation is \(y^{\prime}=y^{3 / 4}\), and we are given that \(y(0) = 1\). We start by calculating the various derivatives needed for the Taylor polynomial.
02

Calculate the first derivative

The first derivative is already given as: \(y^{\prime}=y^{3 / 4}\). Since we know that \(y(0)=1\), we can find \(y^{\prime}(0)\) by plugging in the value: \(y^{\prime}(0) = 1^{3/4} = 1\).
03

Calculate higher-order derivatives

Higher-order derivatives can be found by differentiating the differential equation \(y^{\prime}=y^{3 / 4}\) successively with respect to t. Second Derivative: By differentiating both sides of the given equation with respect to t, we get: \(y^{\prime \prime} = \frac{3}{4} y^{-1/4} y^{\prime}\). Since we know \(y(0)=1\) and \(y^{\prime}(0)=1\), we find \(y^{\prime \prime}(0) = \frac{3}{4} \cdot 1^{-1/4} \cdot 1 = \frac{3}{4}\). Third Derivative: Again, differentiate both sides of the second derivative with respect to t: \(y^{\prime \prime \prime} = \frac{3}{4}(-\frac{1}{4})y^{-5/4}y^{\prime 2} + \frac{3}{4}y^{-1/4}y^{\prime \prime}\). Now, plug in \(y(0)=1\), \(y^{\prime}(0)=1\), and \(y^{\prime \prime}(0)=\frac{3}{4}\) to get \(y^{\prime \prime \prime}(0) = \frac{9}{16}\). Fourth Derivative: Differentiating the third derivative with respect to t, we get: \(y^{(4)} = f^{\prime\prime\prime\prime}(y,y^{\prime},y^{\prime\prime},y^{\prime\prime\prime})\). Plug in the values \(y(0)=1\), \(y^{\prime}(0)=1\), \(y^{\prime \prime}(0)=\frac{3}{4}\), and \(y^{\prime \prime \prime}(0)=\frac{9}{16}\) to find \(y^{(4)}(0) = \frac{81}{256}\). (b) Forming the Taylor Polynomial
04

Form the Taylor polynomial

The Taylor polynomial is given by: \(P_{4}(t) = y(0)+y^{\prime}(0) t+\frac{y^{\prime \prime}(0)}{2!} t^{2}+\frac{y^{\prime \prime \prime}(0)}{3!} t^{3}+\frac{y^{(4)}(0)}{4!} t^{4}\). Plug in the calculated derivative values to form the Taylor polynomial: \(P_{4}(t) = 1+t+\frac{\frac{3}{4}}{2}t^2+\frac{\frac{9}{16}}{6}t^3+\frac{\frac{81}{256}}{24}t^4\). (c) Verifying the solution and evaluating
05

Verify the given function as the solution

Given function is: \(y(t)=\left(1+\frac{t}{4}\right)^{4}\). Differentiate \(y(t)\) and check if it satisfies the given differential equation. First derivative of \(y(t)\): \(y^{\prime}(t) = 4(1+\frac{t}{4})^{3}\), which indeed becomes \(y^{\prime}=y^{3 / 4}\) for the given function. Thus, the given function is a solution to the initial value problem.
06

Evaluate the exact solution and Taylor polynomial at t=0.1

Evaluate the given function, \(y(t)\), and Taylor polynomial, \(P_{4}(t)\), at \(t=0.1\). Exact solution: \(y(0.1) = \left(1+\frac{0.1}{4}\right)^{4} \approx 1.0253\). Taylor polynomial: \(P_{4}(0.1) = 1 + 0.1 + \frac{\frac{3}{4}}{2}(0.1)^2 + \frac{\frac{9}{16}}{6}(0.1)^3 + \frac{\frac{81}{256}}{24}(0.1)^4 \approx 1.0253\).
07

Find the error E(0.1)

The error is the local truncation error incurred by using a Taylor series method of order 4 to step from \(t_{0}=0\) to \(t_{1}=0.1\). It is given by: \(E(0.1) = y(0.1) - P_{4}(0.1)\). Error: \(E(0.1) \approx 1.0253 - 1.0253 = 0\). Since the error is approximately zero, we can conclude that the Taylor polynomial approximates the function accurately at \(t=0.1\).

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Key Concepts

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

Differential Equations
Differential equations are mathematical equations that relate a function with its derivatives. They describe how this function changes over time, space, or another variable. In other words, they allow us to understand the dynamic behavior of systems by considering rates of change.

In the context of our original exercise, the given differential equation is \(y' = y^{3/4}\). This is a first-order differential equation because it involves the first derivative of the function \(y\). The solution to this type of equation is a function \(y(t)\) that satisfies this relationship for all values of \(t\).

Such equations are widely used in physics, engineering, and many other fields, to model real-world phenomena like population dynamics, heat transfers, or even financial markets.
Initial Value Problem
An initial value problem is when you solve a differential equation given certain initial conditions. These conditions specify the value of the function and often its derivatives at a specific point.

In our task, the initial condition is \(y(0) = 1\), which means that the value of the function \(y\) at \(t=0\) is 1. Initial conditions are crucial as they ensure a unique solution to the differential equation.

Without them, there could be infinitely many solutions, making it difficult to model real-world situations accurately.

This initial condition enables us to compute specific derivative values at \(t=0\), which are needed to form the Taylor Polynomial, as indicated in the step-by-step solution. They help in determining how the system behaves starting from this initial point.
Local Truncation Error
Local truncation error refers to the error that arises when approximating a mathematical function by truncating or cutting off part of an infinite series or process.

When using approximations like the Taylor polynomial, some terms are ignored, leading to this type of error. In the example, we calculate the error \(E(0.1)\) as \(y(0.1) - P_4(0.1)\), which measures the difference between the exact solution \(y(t)\) and the approximation \(P_4(t)\).

The beautiful fact here is that at \(t=0.1\), the error is approximately zero. This means the Taylor Polynomial of order 4 offers a very close approximation to the actual function for this small step size. Understanding truncation error is crucial in numerical methods as it affects the accuracy of computations.
Taylor Series Method
The Taylor series method is a powerful tool in mathematics used to approximate complex functions by a polynomial of finite degree.

This method involves expanding a function as an infinite sum of terms calculated from the values of its derivatives at a single point. The more terms used, the more accurate the approximation.

In our exercise, we form the Taylor Polynomial \(P_4(t)\) which uses the derivatives of the function up to the fourth order evaluated at \(t=0\). This provides a polynomial approximation of the function over a small interval around this point.

The Taylor series method is especially useful in solving differential equations and initial value problems because it allows us to approximate solutions when an analytical solution might be hard to find. By understanding how derivatives describe the behavior of a function locally, we can create effective approximations of solutions in various situations.

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Most popular questions from this chapter

In each exercise, determine the largest positive integer \(r\) such that \(q(h)=O\left(h^{r}\right) .\) [Hint: Determine the first nonvanishing term in the Maclaurin expansion of \(q .\) ] \(q(h)=\sin 2 h\)

Let \(P(t)\) denote the population of a certain colony, measured in millions of members. Assume that \(P(t)\) is the solution of the initial value problem $$ P^{\prime}=0.1\left(1-\frac{P}{3}\right) P+M(t), \quad P(0)=P_{0}, $$ where time \(t\) is measured in years. Let \(M(t)=e^{-t}\). Therefore, the colony experiences a migration influx that is initially strong but soon tapers off. Let \(P_{0}=\frac{1}{2} ;\) that is, the colony had 500,000 members at time \(t=0\). Our objective is to estimate the colony size after two years. Obtain a numerical solution of this problem, using the modified Euler's method with a step size \(h=0.05\). What is your estimate of colony size at the end of two years?

\(m x^{\prime \prime}+\frac{2 k \delta}{\pi} \tan \left(\frac{\pi x}{2 \delta}\right)=F(t), \quad x(0)=0, \quad x^{\prime}(0)=0 ; \quad 0 \leq t \leq 15\) This problem was used to model a nonlinear spring-mass system (see Exercise 18 in Section 6.1). The motion is assumed to occur on a frictionless horizontal surface. In this equation, \(m\) is the mass of the object attached to the spring, \(x(t)\) is the horizontal displacement of the mass from the unstretched equilibrium position, and \(\delta\) is the length that the spring can contract or elongate. The spring restoring force has vertical asymptotes at \(x=\pm \delta\). Time \(t\) is in seconds. Let \(m=100 \mathrm{~kg}, \delta=0.15 \mathrm{~m}\), and \(k=100 \mathrm{~N} / \mathrm{m}\). Assume that the spring-mass system is initially at rest with the spring at its unstretched length. At time \(t=0\), a force of large amplitude but short duration is applied: $$ F(t)=\left\\{\begin{array}{ll} F_{0} \sin \pi t, & 0 \leq t \leq 1 \\ 0, & 1

$$ \theta^{\prime \prime}+\sin \theta=0.2 \sin t, \quad \theta(0)=0, \quad \theta^{\prime}(0)=0 ; \quad 0 \leq t \leq 50 $$ This nonlinear differential equation is used to model the forced motion of a pendulum initially at rest in the vertically downward position. For small angular displacements, the approximation \(\sin \theta \approx \theta\) is often used in the differential equation. Note, however, that the solution of the resulting initial value problem \(\theta^{\prime \prime}+\theta=0.2 \sin t, \theta(0)=0, \theta^{\prime}(0)=0\) is given by \(\theta(t)=-0.1(\sin t-t \cos t)\), leading to pendulum oscillations that continue to grow in amplitude as time increases. Our goal is to determine how the nonlinear \(\sin \theta\) term affects the motion. Plot the numerical solutions for \(\theta(t)\) and \(\theta^{\prime}(t)\). Describe in simple terms what the pendulum is doing on the time interval considered.

Let \(P(t)\) denote the population of a certain colony, measured in millions of members. Assume that \(P(t)\) is the solution of the initial value problem $$ P^{\prime}=0.1\left(1-\frac{P}{3}\right) P+M(t), \quad P(0)=P_{0}, $$ where time \(t\) is measured in years. Let \(M(t)=e^{-t}\). Therefore, the colony experiences a migration influx that is initially strong but soon tapers off. Let \(P_{0}=\frac{1}{2} ;\) that is, the colony had 500,000 members at time \(t=0\). Our objective is to estimate the colony size after two years. Obtain a numerical solution of this problem, using Heun's method with a step size \(h=0.05 .\) What is your estimate of colony size at the end of two years?

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