Piecewise Continuous Functions
A function f(t) is said to be piecewise continuous if it has a finite number of discontinuities and does not become infinite at any point. If f(t) is a piecewise continuous function, then its Laplace transform can be defined.
whenever the improper integral converges.
Standard notation: Where the notation is clear, we will use an uppercase letter to indicate the Laplace transform, e.g, L(f; s) = F(s).
The Laplace transform we defined is sometimes called the one-sided Laplace transform. There is a two-sided version where the integral goes from −∞ to ∞.
If f1 (t) ⟷ F1 (s) and [note: ⟷ implies Laplace Transform]
f2 (t) ⟷ F2 (s), then
The step function can take the values of 0 or 1. It is like an on and off switch. The notations that represent the Heaviside functions are uc(t) or u(t-c) or H(t-c)
The bilateral Laplace transform is defined as:
The other way to represent the bilateral Laplace transform is B{F}, instead of F.
The Laplace equation for three-dimensional coordinates can be represented as:
Q1. If f(t) = eat, its Laplace Transform (for s > a) is given by
Solution:
∴ Laplace transform is
Q2. Consider the differential equation
Solution:
Integrating factor =
Solution of y is,
Given that, y(0) = 0
Now, the solution becomes,
Apply Laplace transform
Q3. The Laplace transform of the differential equation y" + ay' + by = f(t). Assume that y(0) = 5, y'(0) = 10, Y(s) and F(s) are the Laplace transforms of y(t) and f(t) respectively
Solution: A second-order differential equation is represented as:
y" + ay' + by = f(t)
The Laplace transform of the above equation with the initial condition is:
Calculation
Given, y(0) = 5, y'(0) = 10
Q4. The inverse Laplace transform of for t ≥ 0 is
Solution: Some pairs of Laplace transforms are given below.
Given:
By applying inverse Laplace transform
⇒ H(t) = e-t + 2t e-t
Q5. If the Laplace transform of function f(t) is given by , then f(0) is
Solution: Laplace Transforms:
Given:
The above equation through partial fractions can be written as:
Comparing co-efficients on both sides, we get
A + B = 1 and 2A + B = 3
We get, A = 2, B = -1
f(t) = 2e-t - e-2tSo,
f(0) = 2e-0 - e-0 = 2 - 1 = 1
∴ f(0) = 1
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