Solve this starting value problem.
Found with the integrating factor and checked in the original equation.
See what kind of equation this is, and what would make it easy
The unknown here is a whole function , and the equation ties its slope to its own value. We cannot simply integrate both sides, because is tangled up on the left with its own derivative. The idea that unlocks it: the left side ALMOST looks like the result of the product rule. If it were exactly the derivative of a product, one integration would finish the job. So we ask what we could multiply by to make it so.
Find the integrating factor
Multiply the equation by an unknown function (the Greek letter mu). The left side becomes . The product rule says . These two match exactly when : a function whose derivative is times itself. Exponentials are the functions that do that.
Multiply through and recognise a product rule
This is the moment the method was designed for. After multiplying by , the left side is no longer two tangled terms; it is the derivative of the single product , and a derivative is something we know how to undo.
Integrate both sides
Integrating the left side simply removes the derivative and leaves . All the real work is on the right: we need a function whose derivative is . A polynomial times an exponential calls for integration by parts, which is the product rule run backwards: it trades the integral for an easier one in which the polynomial has been differentiated away.
Take , so ; and , so . Then:
Divide by the integrating factor
We introduced only as scaffolding. Dividing by it, which is safe because an exponential is never zero, leaves on its own. What appears is a whole family of solutions, one for each value of , and the two parts of it mean different things: one part is forced by the right side of the equation, the other is the free response of the equation itself.
Use the starting value to find the constant
A first order equation has one free constant, and one piece of information fixes it. Without the starting value the equation describes every possible history of the system; the starting value picks out the one that actually happened.
Check the answer in the original equation
A differential equation hands us the perfect test of any proposed answer: differentiate it, put it in, and see whether the two sides agree for EVERY . No trust in the method is required; the check would expose a slip in any of the steps above.