Problem 12
Question
In Problems 11-16, use Euler's Method with \(h=0.2\) to approximate the solution over the indicated interval. $$ y^{\prime}=-y, y(0)=2,[0,1] $$
Step-by-Step Solution
Verified Answer
The approximate solution at \( x = 1.0 \) is \( y = 0.65536 \).
1Step 1: Understanding Euler's Method
Euler's Method is a numerical technique to find approximate solutions to differential equations of the form \( y' = f(x, y) \). It iteratively updates the solution using the formula: \( y_{n+1} = y_n + h imes f(x_n, y_n) \), where \( h \) is the step size.
2Step 2: Initialize Variables
Given the problem, start with the initial condition \( y(0) = 2 \). Set \( x_0 = 0 \) and \( y_0 = 2 \). The step size \( h \) is given as 0.2.
3Step 3: Calculate for x = 0.2
Use Euler's Method to calculate the next value: \( y_1 = y_0 + h imes (-y_0) = 2 + 0.2 imes (-2) = 2 - 0.4 = 1.6 \). Thus, for \( x_1 = 0.2 \), \( y_1 = 1.6 \).
4Step 4: Calculate for x = 0.4
Compute \( y_2 = y_1 + h imes (-y_1) = 1.6 + 0.2 imes (-1.6) = 1.6 - 0.32 = 1.28 \). For \( x_2 = 0.4 \), \( y_2 = 1.28 \).
5Step 5: Calculate for x = 0.6
Compute \( y_3 = y_2 + h imes (-y_2) = 1.28 + 0.2 imes (-1.28) = 1.28 - 0.256 = 1.024 \). For \( x_3 = 0.6 \), \( y_3 = 1.024 \).
6Step 6: Calculate for x = 0.8
Compute \( y_4 = y_3 + h imes (-y_3) = 1.024 + 0.2 imes (-1.024) = 1.024 - 0.2048 = 0.8192 \). For \( x_4 = 0.8 \), \( y_4 = 0.8192 \).
7Step 7: Calculate for x = 1.0
Compute \( y_5 = y_4 + h imes (-y_4) = 0.8192 + 0.2 imes (-0.8192) = 0.8192 - 0.16384 = 0.65536 \). For \( x_5 = 1.0 \), \( y_5 = 0.65536 \).
Key Concepts
Numerical ApproximationDifferential EquationsInitial Value Problem
Numerical Approximation
Numerical approximation is a crucial tool in mathematics, especially when solving complex problems where an exact analytical solution is difficult to achieve or does not exist. It involves finding approximate solutions by using simpler arithmetic calculations.
One common method of numerical approximation is Euler's Method. This approach helps us approximate solutions to differential equations by making small steps along the function graph, rather than attempting to solve the equation exactly. This is particularly useful for differential equations that do not have simple, closed-form solutions.
One common method of numerical approximation is Euler's Method. This approach helps us approximate solutions to differential equations by making small steps along the function graph, rather than attempting to solve the equation exactly. This is particularly useful for differential equations that do not have simple, closed-form solutions.
- To use Euler's Method, you need an initial value, a specified interval, and a chosen step size, denoted as \( h \).
- Euler’s formula, \( y_{n+1} = y_n + h \times f(x_n, y_n) \), allows you to iteratively find the next point.
Differential Equations
Differential equations are equations that involve an unknown function and its derivatives. They play a fundamental role in describing various phenomena in engineering, physics, economics, biology, and more.
For example, a simple differential equation can express the rate at which a population grows or decays. The equation \( y' = -y \) from our exercise tells us that the rate of change of the function \( y \) is proportional to the negative of the function itself. This is known as an exponential decay differential equation.
For example, a simple differential equation can express the rate at which a population grows or decays. The equation \( y' = -y \) from our exercise tells us that the rate of change of the function \( y \) is proportional to the negative of the function itself. This is known as an exponential decay differential equation.
- Differential equations are categorized based on the highest order of derivative present and the linearity of the equation.
- They can be solved by analytical methods, yielding exact solutions, or by numerical methods, like Euler's Method, for approximate solutions.
Initial Value Problem
An initial value problem (IVP) is a type of differential equation accompanied by specified initial conditions. It is crucial because it defines the starting point from which a solution is sought.
In practice, the initial condition \( y(x_0) = y_0 \) specifies the value of the solution at a particular point \( x_0 \). In our exercise, this is given as \( y(0) = 2 \), which means when \( x = 0 \), \( y \) starts at 2. This problem-solving technique is common for modeling time-evolving systems where the initial state or condition heavily influences future behavior.
In practice, the initial condition \( y(x_0) = y_0 \) specifies the value of the solution at a particular point \( x_0 \). In our exercise, this is given as \( y(0) = 2 \), which means when \( x = 0 \), \( y \) starts at 2. This problem-solving technique is common for modeling time-evolving systems where the initial state or condition heavily influences future behavior.
- IVPs are solved by integrating the differential equation with respect to the initial conditions.
- Essentially, an initial condition provides the specific solution to the differential equation from the family of solutions that exist.
Other exercises in this chapter
Problem 12
In Problems 1-12, evaluate the given integral. $$ \int_{0}^{2 \pi}|\sin 2 x| d x $$
View solution Problem 12
In Problems 1-54, perform the indicated integrations. \(\int_{-\pi / 4}^{9 \pi / 4} e^{\cos z} \sin z d z\)
View solution Problem 12
In Problems 1-28, perform the indicated integrations. \(\int \cos ^{6} \theta \sin ^{2} \theta d \theta\)
View solution Problem 12
\(\int_{2}^{3} \frac{d t}{t^{2} \sqrt{t^{2}-1}}\)
View solution