Solving the Convolution Integral Using Unit Step Functions
Solving the Convolution Integral Using Unit Step Functions
Convolution integrals are commonly encountered in various fields, such as signal processing, control theory, and systems analysis. This article provides a detailed step-by-step solution to the convolution integral:
It integral-∞∞ e-2τ u(t - τ) e-(t - τ) u(τ) dτ
Role of Unit Step Functions
First, let's clarify the role of the unit step functions used in this problem. The functions u(t - τ) and u(τ) are defined as follows:
u(t - τ) is 0 for τ ≤ 0 and 1 for τ 0. u(τ) is 0 for τ ≤ 0 and 1 for τ 0.Therefore, the integration will only take place over the interval where both step functions are 1. From the definitions of these functions, this interval is given by:
0 ≤ τ ≤ t
Rewriting the Integral
With the interval determined, we can now rewrite the convolution integral as follows:
It integral0t e-2τ e-(t - τ) dτ
Simplifying the Integrand
To simplify the integrand, we multiply the exponential functions:
e-2τ e-(t - τ) e-2τ e-t eτ e-t e-τ
Substituting this into the integral, we obtain:
It e-t integral0t e-τ dτ
Evaluating the Integral
Next, we evaluate the integral integral0t e-τ dτ:
integral0t e-τ dτ -e-τ |0t -e-t - (-e0) 1 - e-t
Substituting this back into the expression for It, we get:
It e-t (1 - e-t) e-t - e-2t
Thus, the solution to the convolution integral is:
Final Solution
boxed{e-t - e-2t}
Implications and Visualization
This result can be further interpreted visually. The convolution integral effectively considers the overlap of the two step functions u(t - τ) and u(τ). For a fixed value of t, the product of the two step functions is non-zero only when both are 1, which occurs for 0 ≤ τ ≤ t.
Consider a different representation of the convolution integral:
It e-t integral-∞∞ e-τ u(t - τ) u(τ) dτ
Using the properties of unit step functions, we can simplify the integral as follows:
u(t - τ) u(τ) 0 for τ ≤ 0 and τ ≥ t, and 1 for 0 ≤ τ ≤ t
This results in the integral:
It e-t integral0t e-τ dτ e-t (1 - e-t) e-t - e-2t
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