1. Inversion of the Laplace transform
The Laplace transform of a function f (t) of a function of exponential order is defined as
F(s) = ∫∞
e−st f (t) dt.
This transform had many applications in applied mathematics. It can be shown that the inverse
transform can be obtained as the Bromwich integral,
f (t) = 1
2πi ∫γ + i∞
γ − i∞
ezt F(z) dz.
The integrand here is over the line where is chosen sufficiently large that all
singularities of lie to the left of the line. In practice we evaluate the integral as the limit as
of a contour integral over the contour shown below. Note that the curved part is a
semicircle of radius centred on the point , not . We assume throughout that is
Re (z) = γ γ
R → ∞
R z = γ z = 0 t
Re( z )
Im( z )
The Bromwich contour
We are going to use this contour to evaluate the inverse transform of two functions. Both of
these can be done easily by elementary methods, but they serve to illustrate the method.
F(s) = 1
(s + 1)2 + 1
Since the poles of this are in the left half plane, we can chose γ = 0.
Use the Residue Theorem to find f (t).
Note that to obtain full marks you must give a proper proof that the integral around the curved
section of the Bromwich contour tends to zero as goes to infinity. In particular, you need to
find the maximum value of on the contour.
Recently Asked Questions
- Please refer to the attachment to answer this question. This question was created from CHAPTER 8,9,10,13.
- Matt ( m = 80 kg) and Trey ( m = 90 kg) slide across an ice skating rink and collide with each other. Before the collision, Matt was moving 3 m/s to the
- Analyze and explain the impact of the proliferation of mobile devices on cloud-based computing in various industries. For example, the rise of mobile phones