This is represented by the formula E = ∫|x(t)|^2 dt from -∞ to ∞, where x(t) is the signal.
For the signals in Fig. 1.3a, 1.3b, 1.3c, and 1.3d, we are given their energies as 4, 1, 4/3, and 4/3, respectively. This means that when we apply the formula to these
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