Chapter 2: Problem 15
find the solution of the given initial value problem. $$ t y^{\prime}+2 y=t^{2}-t+1, \quad y(1)=\frac{1}{2}, \quad t>0 $$
Short Answer
Step by step solution
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Initial Value Problem
\( t y^{\prime}+2 y=t^{2}-t+1 \)
and the initial condition:
\( y(1)=\frac{1}{2} \).
- The equation is solved for a specific value of the function \( y(t) \) at \( t = 1 \).
- The purpose of the initial condition is to find the particular solution that fits the specific requirement of \( y \) when \( t \) equals the given initial value.
Integrating Factor
\( y^{\prime} + P(t)y = Q(t) \),
An integrating factor \( \mu(t) \) is calculated, transforming the differential equation into an exact equation.
- Begin by identifying \( P(t) \) from the equation.
- Calculate the integrating factor, \( \mu(t) = e^{\int P(t) \, dt} \).
\( y^{\prime} + \frac{2}{t}y = \frac{t^{2}-t+1}{t} \),
where \( P(t) = \frac{2}{t} \).
The integrating factor hence is:
\( \mu(t) = e^{\int \frac{2}{t} \, dt} = t^2 \).
Multiplying the equation with this factor facilitates the integration of both sides and transforms the equation into an exact differential, allowing easier integration.
Exact Differential Equation
For the equation
\( t^2 y^{\prime}+2t y = t^{3}-t^{2}+t \),
an integrating factor has transformed it to:
\( \frac{d}{dt}(t^2 y) = t^3 - t^2 + t \).
- The left-hand side \( \frac{d}{dt}(t^2 y) \) represents the derivative of the product \( t^2 y \).
- This makes the equation straightforward to solve by integrating both sides with respect to \( t \).
\( t^2 y = \frac{1}{4}t^4 - \frac{1}{3}t^3 + \frac{1}{2}t^2 + C \).
This integration step works because the differential form reflects an exact derivative, thus easing up the task of finding the particular solution by direct integration.
Particular Solution
- In our example, the general solution was found to be:
- \( y(t) = \frac{1}{4}t^2 - \frac{1}{3}t + \frac{1}{2} + \frac{C}{t^2} \).
\[ \frac{1}{2} = \frac{1}{4} - \frac{1}{3} + \frac{1}{2} + C \].
By solving for \( C \), you find \( C = 0 \), giving the particular solution:
\( y(t) = \frac{1}{4}t^2 - \frac{1}{3}t + \frac{1}{2} \).
The unique aspect of the particular solution is that it satisfies both the equation and the initial condition, providing a specific application of the general solution for a scenario.