Enter either a function or an ordinary differential equation (ODE) to calculate the Laplace transform with clear, step-by-step solution.
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Use this Laplace transform calculator to find the Laplace transformation of a function f(t) or ordinary differential equation (ODE). Our calculator uses relevant Laplace transform formulas and integral operations to provide precise results with detailed steps.
Laplace transform is a mathematical technique that is used to convert a function f(t) into a function of complex variable(s). This technique is widely used in physics, engineering and control theory to solve ordinary differential equations (ODE's).
Mathematically,
\(F(s) = \int_{0}^{∞} f(t)e^{-st} dt\)
Where;
There are two possible methods to find Laplace transforms:
\(F(s) = \int_{0}^{∞} f(t)e^{-st} dt\)
Example:
Suppose we have the function given below:
\(f(t)=6e^{-5t}+e^{3t}+5t^{3}-9\)
Step 01: Write down the Laplace transform formula
\(F(s) = \int_{0}^{∞} f(t)e^{-st} dt\)
Step 02: Input the given function f(t)
\(F(s) = \int_{0}^{∞} f(t)e^{-st} dt\) \(F(s) = \int_{0}^{∞} (6e^{-5t}+e^{3t}+5t^{3}-9) e^{-st} dt\)
Step 03: Apply the formula to individual terms
\(\int_{0}^{∞} 6e^{-5t} e^{-st} dt\) \(=6\int_{0}^{∞} e^{-(5+s)t} dt\) \(=6[\dfrac{1}{-(5+s)}e^{-(5+s)t}]_{0}^{∞}\) \(=6[\dfrac{1}{s+5}]\)
\(\int_{0}^{∞} e^{3t} e^{-st} dt\) \(=\int_{0}^{∞} e^{(3-s)t}dt\) \(=[\dfrac{1}{3-s}e^{(3-s)t}]_{0}^{∞}\) \(=\dfrac{1}{s-3}\)
\(\int_{0}^{∞} 5t^{3} e^{-st} dt\) \(=5\int_{0}^{∞}t^{3}e^{-st}dt\) \(=[\dfrac{1}{3-s}e^{(3-s)t}]_{0}^{∞}\) \(=5*\dfrac{3!}{s^{4}}\) \(=\dfrac{30}{s^{4}}\)
\(\int_{0}^{∞} -9 e^{-st} dt\) \(=-9\int_{0}^{∞} e^{-st} dt\) \(=-9[\dfrac{-1}{s}e^{-st}]_{0}^{∞}\) \(=\dfrac{9}{s}\)
Step 04: Sum up all transforms together
\(F(s)=6(\dfrac{1}{s+5}+\dfrac{1}{s-3}+\dfrac{30}{s^{4}}-\dfrac{9}{s})\)
To convert back this function to the original time domain equation, you can use our inverse Laplace transform calculator.
The following Laplace transform table helps you to find the Laplace Transformation of simple and most common functions:
Function name | Time-domain function | Laplace transforms online |
f (t) | F(s) = L{f (t)} | |
Constant | 1 | 1/s |
Linear | t | 1/\(s^2\) |
Power | t n | n!/\(s^{n+1}\) |
Power | t a | Γ(a+1) ⋅ s -(a+1) |
Exponent | e at | 1/s-a |
Sine | sin at | a/ \(s^2 + a^2\) |
Cosine | cos at | s/ \(s^2 + a^2\) |
Hyperbolic sine | sinh at | a/ \(s^2 - a^2\) |
Hyperbolic cosine | cosh at | s/ \(s^2 - a^2\) |
Growing sine | t sin at | 2as/ \((s^2 + a^2)^2\) |
Growing cosine | t cos at | \(s^2 - a^2/ (s^2 + a^2)^2\) |
Decaying sine | e -at sin ωt | ω /\((s+a)^2 + ω^2\) |
Decaying cosine | e -at cos ωt | (s+a)/\((s+a)^2 + ω^2\) |
Delta function | δ(t) | 1 |
Delayed delta | δ(t-a) | e-as |
Our online Laplace transform calculator automates the transformations of functions based on the following properties:
Property | Equation |
---|---|
Linearity | F(s) = L{f(t)} + L{g(t)} |
Time Delay | L{f(t-td)} = e^(-tsd) F(s) |
First Derivative | L{f'(t)} = sF(s) - f(0-) |
Second Derivative | L{f''(t)} = s^2 F(s) - sf(0-) - f'(0-) |
Nth Derivative | L{f^(n)(t)} = s^n F(s) - s^(n-1)f(0-) - ... - f^(n-1)(0-) |
Integration | L{∫f(t) dt} = 1/s F(s) |
Convolution | L{f(t) * g(t)} = F(s)G(s) |
Initial Value Theorem | lim(s->∞) sF(s) = f(0-) |
Final Value Theorem | lim(s->0) sf(s) = f(∞) |
Laplace calculator has vast applications in various fields including:
Using the Laplace Transform you can convert a time-domain signal into a complex frequency domain signal. On the other hand, the Fourier Transforms convert the same signal into a ‘jw’ (complex frequency) plane. It is also the subset of Laplace transform, especially when the real part of the frequency is ‘0’.
Yes, it can be. If you have a function f(t)=0, then its Laplace transform F(s)=0 can be determined by multiplying the Laplace pair with a scalar 0, which defines the linearity property. It means the transformation of a scalar multiple is the scalar multiplication of the transformed function.
From the source of Wikipedia: Formal definition, Bilateral Laplace transform, Inverse Laplace transform.
From the source of Paul's Online Notes: Laplace Transforms, Solving IVPs with Laplace Transforms, Nonconstant Coefficient IVP’s.
From the source of Swarth More: Linearity, Time Delay, First Derivative, Second Derivative, Initial Value Theorem, Final Value Theorem.
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