The formula this page uses
F(s) = ∫₀^∞ e^(−st) f(t) dt L{y′} = s·Y(s) − y(0)
Solve laplace transform problems with clear steps, notation, and a final check.
Evaluate the governing formula locally in your browser. Define each known quantity once, then change values to test another case instantly.
Choose an example or enter a formula.
No calculations yet.
F(s) = ∫₀^∞ e^(−st) f(t) dt L{y′} = s·Y(s) − y(0)
The function
Because it converts calculus into algebra. y′ + 3y = 0 becomes sY − 4 + 3Y = 0, which is one line of rearranging. It also swallows the initial condition automatically, instead of leaving a constant C to pin down at the end.
It is a complex frequency. The real part measures how fast something grows or decays, and the imaginary part measures oscillation. The pole at s = −3 above is exactly the −3 in the decay e^(−3t).
The defining integral ∫₀^∞ e^(−st) f(t) dt only converges when e^(−st) shrinks faster than f(t) grows. For e^(2t) you need s > 2, and below that the transform simply does not exist.
Factor the denominator and split with partial fractions: 4/((s+2)(s+3)) = 4/(s+2) − 4/(s+3). Each piece is now a table row, giving y(t) = 4e^(−2t) − 4e^(−3t).