Chapter 15: Problem 6
Solve the following first-order linear differential equations; if an initial condition is given, definitize the arbitrary constant: $$\frac{d y}{d t}+y=t$$
Short Answer
Expert verified
The solution of the differential equation is \( y = t - 1 + Ce^{-t} \).
Step by step solution
01
Identify the Standard Form of Linear Differential Equation
First, recognize that the given equation \( \frac{d y}{d t} + y = t \) is a first-order linear differential equation of the form \( \frac{d y}{d t} + P(t)y = Q(t) \). Here, \( P(t) = 1 \) and \( Q(t) = t \).
02
Find the Integrating Factor
For a linear differential equation, the integrating factor \( \mu(t) \) is given by \( e^{\int P(t) \, dt} \). Here, \( P(t) = 1 \), so \( \int P(t) \, dt = \int 1 \, dt = t \). Thus, \( \mu(t) = e^t \).
03
Multiply the Equation by the Integrating Factor
Multiply the entire differential equation by the integrating factor \( e^t \). This gives: \[ e^t \frac{d y}{d t} + e^t y = t e^t \].
04
Simplify to Find the Left-Hand Side
Notice that the left-hand side of the equation can be written as the derivative of a product: \[ \frac{d}{d t}(e^t y) = e^t \frac{d y}{d t} + e^t y \]. So the equation becomes: \[ \frac{d}{d t}(e^t y) = t e^t \].
05
Integrate Both Sides
Integrate both sides with respect to \( t \): \[ \int \frac{d}{d t}(e^t y) \, dt = \int t e^t \, dt \]. The left-hand side simplifies to \( e^t y \), and the integral on the right-hand side can be solved using integration by parts. Let \( u = t \) and \( dv = e^t \, dt \), then \( du = dt \) and \( v = e^t \). Integration by parts formula \( \int u \, dv = uv - \int v \, du \) gives: \[ \int t e^t \, dt = t e^t - \int e^t \, dt = t e^t - e^t + C \]. Thus, \[ e^t y = t e^t - e^t + C \].
06
Solve for y
Solve the equation \( e^t y = t e^t - e^t + C \) for \( y \) by dividing every term by \( e^t \): \[ y = t - 1 + Ce^{-t} \].
07
Apply Initial Condition (If Given)
If an initial condition is specified, such as \( y(0) = y_0 \), substitute \( t = 0 \) and \( y = y_0 \) into the solution to determine the constant \( C \). If no initial condition is provided, \( C \) remains arbitrary.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
First-order linear differential equations
A first-order linear differential equation is a type of equation that involves two main components: a function and its derivative. These equations follow a standard form, which is crucial to identify when you begin solving. The form is given by \[ \frac{d y}{d t} + P(t)y = Q(t) \] Understanding this structure helps you apply systematic methods to solve the equation. In this form,
- \( y \) is the function you want to find,
- \( \frac{d y}{d t} \) is its derivative with respect to \( t \),
- \( P(t) \) and \( Q(t) \) are known functions of \( t \).
Integrating factor
One powerful technique to solve first-order linear differential equations is using an integrating factor. This method transforms a difficult equation into one that is much easier to solve.Here's how it works step-by-step:
- Determine the integrating factor \( \mu(t) \) using the formula \( e^{\int P(t) \, dt} \).
- In our example, \( P(t) = 1 \), so the integral is simply \( t \), leading to the integrating factor \( \mu(t) = e^t \).
- Multiply every term in the differential equation by \( \mu(t) \). This rewrites the left-hand side as the derivative of a product.
Integration by parts
Once the integrating factor simplifies the equation, you might be left with integrals that need special techniques to solve. For integration involving products of functions, **integration by parts** is a key tool.The integration by parts formula is: \[ \int u \, dv = uv - \int v \, du \] Where you choose:
- \( u \) and \( dv \)
- Find their derivatives \( du \) and \( v \)
- Set \( u = t \) and \( dv = e^t \, dt \) leading to \( du = dt \) and \( v = e^t \).
- This transforms the integral \( \int t e^t \, dt \) into \( t e^t - \int e^t \, dt \).
Initial condition
An **initial condition** provides specific values for the function at a certain point, narrowing down the infinite possibilities into a single, unique solution.Given a general solution for a first-order linear differential equation:
- The constant \( C \) appears in the solution due to the integration process.
- If an initial condition is given, like \( y(0) = y_0 \), substitute these values to solve for \( C \).
- If \( y(0) = y_0 \), plug in \( t = 0 \), and \( y = y_0 \) into the general solution \( y = t - 1 + Ce^{-t} \).
- Isolating \( C \) will render a specific solution tailored to this initial scenario.