How one multiplier turns a linear differential equation into a product derivative.
By Theory Commons Editors4 min readPublished Aug 22, 2026
A linear first-order equation has standard form
y′+p(t)y=q(t).
Multiplying by
μ(t)=e∫p(t)dt
makes the left side equal to (μy)′.
The method
After multiplication,
μy′+μpy=μq=(μy)′.
Integrate and solve:
y=μ1(∫μqdt+C).
Any nonzero constant factor in μ cancels, so the simplest antiderivative is sufficient.
Derive the factor instead of memorizing it
Multiply y′+p(t)y=q(t) by an unknown function μ(t). We want
μy′+μpy=(μy)′=μy′+μ′y.
Matching coefficients of y requires μ′=pμ. Separating this auxiliary equation gives μ=e∫p(t)dt. The formula follows directly from the product rule.
Interpret the two pieces
The term 3 is the equilibrium response to the constant input. The term −2e−2t is a transient that carries the initial mismatch and decays. This steady-plus-transient decomposition is often more informative than the formula alone.
Check your understanding
What integrating factor belongs to ty′+2y=t3 on t>0?
Show the reasoning
First divide by t: y′+(2/t)y=t2. Thus μ=e∫2/tdt=e2lnt=t2 for t>0.