Chapter 4: Problem 14
\(y^{\prime}=y \cos (t)\), with \(y(0)=1\), on \([0,2 \pi]\).
Short Answer
Expert verified
The solution is \(y = e^{\sin(t)}\) for \(t \in [0, 2\pi]\).
Step by step solution
01
Identify the Type of Differential Equation
The given differential equation is \(y' = y\cos(t)\). This is a first-order linear differential equation since it can be written in the form \(y' = f(t) y\).
02
Use the Separation of Variables Method
For the equation \(y' = y \cos(t)\), separate variables by dividing both sides by \(y\) and multiplying by \(dt\): \(\frac{dy}{y} = \cos(t) \, dt\).
03
Integrate Both Sides
Integrate the left-hand side with respect to \(y\) and the right-hand side with respect to \(t\):\[\int \frac{dy}{y} = \int \cos(t) \, dt\]This leads to \(\ln |y| = \sin(t) + C\), where \(C\) is the constant of integration.
04
Solve for \(y\)
Exponentiate both sides to get rid of the natural logarithm:\[ |y| = e^{\sin(t) + C}\]Since \(y\) is positive (from the initial condition), we simplify this to:\[ y = e^C e^{\sin(t)}\]Let \(A = e^C\), so \(y = A e^{\sin(t)}\).
05
Apply the Initial Condition
Apply the initial condition \(y(0)=1\) to find \(A\):\[ y(0) = A e^{\sin(0)} = A imes e^0 = A = 1\]Thus, \(A = 1\) and the solution becomes \(y = e^{\sin(t)}\).
06
Ensure Solution Validity on the Given Interval
The solution \(y = e^{\sin(t)}\) is valid for all \(t\) in the interval \([0, 2\pi]\) since sine and exponentials are defined everywhere for real numbers.
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Separation of Variables
Separation of Variables is a fundamental technique used to solve differential equations. It involves separating the variables in an equation so that each variable is on a different side of the equation. In the problem at hand, the equation is given as \(y' = y \cos(t)\). By applying this method, we attempt to isolate \(y\) on one side and \(t\) on the other.
In our example, we rewrite the equation to isolate \(dy\) and \(dt\):
In our example, we rewrite the equation to isolate \(dy\) and \(dt\):
- Divide both sides by \(y\): \(\frac{dy}{y} = \cos(t) \ dt\).
- We now have an equation where the left side contains only the \(y\) variable and the right side contains only \(t\).
First-order Linear Differential Equation
A first-order linear differential equation is a type of differential equation characterized by the presence of the first derivative of the unknown function and that derivative being linear. The general form looks like \(y' + p(t)y = q(t)\). Here, \(p(t)\) and \(q(t)\) are functions of \(t\), but \(y'\) is first-order and linear.
In our specific case, the differential equation \(y' = y \cos(t)\) fits the criteria for a first-order linear equation, especially since it rearranges to \(y' - y \cos(t) = 0\) by comparing to its general form. Recognizing this helps determine the suitable solving method, which includes separation of variables when \(p(t)\) is constant or simple in structure. Linear first-order equations often have predictable behaviors, making their solutions analytically convenient.
In our specific case, the differential equation \(y' = y \cos(t)\) fits the criteria for a first-order linear equation, especially since it rearranges to \(y' - y \cos(t) = 0\) by comparing to its general form. Recognizing this helps determine the suitable solving method, which includes separation of variables when \(p(t)\) is constant or simple in structure. Linear first-order equations often have predictable behaviors, making their solutions analytically convenient.
Initial Value Problem
The Initial Value Problem (IVP) gives us more than just a differential equation—it also provides specific conditions that the solution must satisfy at a given point. For the provided exercise, we are given \(y(0) = 1\), which defines the state of the function \(y(t)\) at \(t = 0\).
Solving an IVP typically involves two main steps:
Solving an IVP typically involves two main steps:
- First, solve the differential equation generally, leaving it in terms of an arbitrary constant \(C\).
- Next, substitute the initial conditions to find \(C\), thereby arriving at a specific solution.
Mathematical Integration
Mathematical Integration is a crucial step in solving differential equations, particularly when using separation of variables. It involves finding the integral, or the anti-derivative, of a function. Integration is used to reverse the process of differentiation, allowing us to go from a derivative back to a function.
In the provided exercise, once variables are separated, we face the task of integrating:
In the provided exercise, once variables are separated, we face the task of integrating:
- The left side, \(\int \frac{dy}{y}\), which results in \(\ln |y|\).
- The right side, \(\int \cos(t) \, dt\), which leads to \(\sin(t) + C\), introducing a constant of integration.