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  1. The transfer function for the continuous-time system relates the Laplace transform of the continuous-time output to that of the continuous-time input described by LTI differential …

  2. We’ve just seen how time-domain functions can be transformed to the Laplace domain. Next, we’ll look at how we can solve differential equations in the Laplace domain and transform back to …

  3. In this chapter we introduce the Fourier transform and review some of its basic properties. The Fourier transform is the \swiss army knife" of mathematical analysis; it is a powerful general …

  4. The z-transform is a generalization of the Fourier transform, the principal motivation for introducing the generalization is that the Fourier transform does not converge for all …

  5. 1 df is called the inverse Fourier transform of X(f ). Notice that it is identical to the Fourier transform except for the sign in the exponent of the complex exponential.

  6. First find the s-domain equivalent circuit... then write the necessary mesh or node equations. When analyzing a circuit with mutual inductance it is necessary to first transform into the T …

  7. The Fourier transform of f ̃(ω) = 1 gives a function f(t) = δ(t) which corresponds to an infinitely sharp pulse. For a pulse has no characteristic time associated with it, no frequency can be …