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  1. 1. The idea. We turn our attention now to transform methods, which will provide not just a tool for obtaining solutions, but a framework for understanding the structure of linear ODEs. The idea is to de ne a transform operator L on functions, L : origin space ! transformed space. such that the ODE in the transformed space is much easier to solve.

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  2. 4.1 Definition and the Laplace transform of simple functions. Given f, a function of time, with value f(t) at time t, the Laplace transform of f which is. denoted by L(f) (or F ) is defined by. F (s) = e st. (t.

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  3. SUMMARY OF THE LAPLACE TRANFORM. The Laplace Transform of a function f ( t ) , t ≥ 0 is defined as. ∫. ∞. L − f ( t ) ≡ f ( s ) ≡ e st f ( t ) dt , 0. where s ∈C , with Re ( s ) sufficiently large for the integral to converge. The Laplace Transform is a linear operation.

  4. Transform rule: The Laplace transform has a number of nice standard transforms, very similar to the Fourier transform. A few are listed below (proofs left as exercises).

  5. The Laplace Transform is a critical tool used in the theory of diferential equations with important applications to fields such as electrical engineering. Despite its many applications, the transform is mathematically rich, leading to several important theorems considering its behavior on diferent functions and its own structure.

  6. The Laplace transform of the derivative of a function is the Laplace transform of that function multiplied by 𝑠𝑠minus the initial value of that function. ℒ𝑔𝑔̇𝑡𝑡= 𝑠𝑠𝐺𝐺𝑠𝑠−𝑔𝑔(0) (3)

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  8. The Laplace transform. we'll be interested in signals de ̄ned for t ̧ 0 L(f = ) the Laplace transform of a signal (function) de ̄ned by Z f is the function F. (s) = f (t)e¡st dt. 0. for those s 2 C for which the integral makes sense. 2 F is a complex-valued function of complex numbers.

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