Laplace transform definition

Equation 2.28 is the Laplace transform of Equation 2.27. EXAMPLE 2.6 

Laplace transforms of some commonly occurring functions in oil and gas industry system safety and reliability-related analysis studies are presented in Table 2.1 [10-12]. 

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Laplace Transform Definition, Common Laplace Transforms, and Final-Value Theorem... 

The results in the Laplace domain can also be used to obtain results in the time domain. To this end, we first note that setting 5 = ico, with co the Fourier frequeney, in the Laplace transform definition yields... 

We will obtain some Laplace transforms by applying the definition, Eq. (3-65). Suppose F(t) = a, where a is a constant. Then... 

Application of the definition shows that the Laplace transform is a linear oper-ator " this property is represented in Eqs. (3-67) and (3-68). 

Derivatives 35. Maxima and Minima 37. Differentials 38. Radius of Curvature 39. Indefinite Integrals 40. Definite Integrals 41. Improper and Multiple Integrals 44. Second Fundamental Theorem 45. Differential Equations 45. Laplace Transformation 48. 

The Laplace transform of a time-dependent variable X(t) is denoted by Lap X t) or x(5) and is defined by means of the definite integral over the positive time domain ... 

The rectangular pulse can be generated by subtracting a step function with dead time T from a step function. We can derive the Laplace transform using the formal definition... 

Consider the definition of the Laplace transform of a derivative. If we take the limit as 5 approaches zero, we find... 

This is just a simple matter of substituting the definition of Laplace transform. 

Hence, we can view the transfer function as how the Laplace transform of the state transition matrix O mediates the input B and the output C matrices. We may wonder how this output equation is tied to the matrix A. With linear algebra, we can rewrite the definition of O in Eq. (4-5) as... 

The solution of Eq. (78) can be obtained with the use of the Laplaee transform. However, it is first necessary to develop the expression for the Laplace transform of the delta function, as given on the right-hand side of Eq. (78). With the use of the definition of the Laplace transform [Eq. (43)] and f(t) = (t -t ), the desired result becomes... 

This involves obtaining the mean-residence time, 0, and the variance, (t, of the distribution represented by equation 19.4-14. Since, in general, these are related to the first and second moments, respectively, of the distribution, it is convenient to connect the determination of moments in the time domain to that in the Laplace domain. By definition of a Laplace transform,... 

If we then notice that the bracketed expression in the first integral of (65 ) is nothing else but the Laplace transform of PoKP> t)>we obtain, applying the well-known convolution theorem of Laplace transforms together with the definitions (64) and (65),... 

Moreover, using the definition (10) of the streaming operator Sf and the perturbation expansion of its Laplace transform Rn(z) (see 28), it is easy to show that... 

Let us now apply the definition of the Laplace transformation to some important time functions steps, ramps, exponential, sines, etc. 

The integral is, by definition, just the Laplace transformation of X( , which we call... 

We denote the fluctuations of the number density of the monomers of component j at a point r and at a time t as pj r,t). With this definition we have pj(r,t))=0. In linear response theory, the Fourier-Laplace transform of the time-dependent mean density response to an external time dependent potential U r,t) is expressed as ... 

From the definition of the Laplace transform, Eq. (11.28), it is straightforward to show that it replaces a differential operator d/dt by the Laplace variable s (see Appendix G for details). The feedback circuit is typically an amplifier with an RC network, as shown in Fig. 11.6. The RC network is used for compensation, which will be explained here. By denoting the Laplace transform of the voltage on the z piezo, Vz(t), by U(s), the Laplace transform of the feedback circuit is... 

Fermi-level DOS 115 Jellium model 92—97 failures 97 schematic 94 surface energy 96 surface potential 93 work function 96 Johnson noise 252 Kohn-Sham equations 113 Kronig-Penney model 99 Laplace transforms 261, 262, 377 and feedback circuits 262 definition 261 short table 377 Lateral resolution... 

Consider first the series junction of N waveguides containing transverse force and velocity waves. At a series junction, there is a common velocity while the forces sum. For definiteness, we may think of A ideal strings intersecting at a single point, and the intersection point can be attached to a lumped load impedance Rj (s), as depicted in Fig. 10.11 for TV= 4. The presence of the lumped load means we need to look at the wave variables in the frequency domain, i.e., V(s) = C v for velocity waves and F(s) = C / for force waves, where jC denotes the Laplace transform. In the discrete-time case, we use the z transform instead, but otherwise the story is identical. 

Inserting the Laplace transformation of Eq. (3.34) into Eq. (3.13), we get the general DET definition of ideal Stern-Volmer constant ... 

The boundary conditions for both are the same the Laplace transformed Eqs. (3.121). To obtain the kernels from the solutions of Eqs. (3.122) and (3.123), one should insert them into the memory function definitions (3.116) adopted to the contact reactions ... 

Taking into account the definitions given for the Laplace transforms of the kernels in Eqs. (3.382), (3.386), and (3.389), we can put the stationary IET equations in exactly the same form as in the Markovian theory ... 

It is remarkable that the integral equation (3.693) proved to be formally exact [51], so that all theories differ only in their definition of the kernel, given as E(f) or V(.v). Sometimes the kernel is explicitly defined in the original works, but more often the reduction to the integral form and extraction of the kernel is a separate problem solved in Ref. 46. In a few cases this procedure was nontrivial and required rather long and sophisticated calculations that are of no interest except for the final results represented by the Laplace transformed kernels S in Table V. 

Since 0 < a < 1 the exponent in Eq. (137) is 1 — a > 0. The mathematical implication is that M(p) (137) is a multivalued function of the complex variable p. In order to represent this function in the time domain, one should select the schlicht domain using supplementary physical reasons [135]. These computational constraints can be avoided by using the Riemann-Liouville fractional differential operator oDlt a [see definitions (97) and (98)]. Thus, one can easily see that the Laplace transform of... 

To convince the reader that Eq. (243) is a proper expression for the memory kernel of infinite age, it is enough to show that this approach to the stationary correlation function 3L(t) yields the same result as the prediction of the renewal arguments, namely, Eq. (147). To prove this important fact, we use the definition of the infinitely aged memory kernel given by Eq. (243), we plug it in Eq. (247) and we compare the resulting expression with the Laplace transform of Eq. (147) so as to assess whether we get the same analytical expression. 

The characteristic function for a distribution law of a random variable is the Laplace transform of the expression of the distribution law. For the analysis of the properties of the distribution of a random variable, the characteristic function is good for the rapid calculation of the centred or not, momentum of various orders. Here below, we have the definition of the characteristic function cp (s) and its particularization with the case under discussion ... 

Ignition processes often are characterized by a gradual increase of temperature that is followed by a rapid increase over a very short time period. This behavior is exhibited in the present problem if a nondimensional measure of the activation energy E is large, as is true in the applications. Let tc denote an ignition time, the time at which the rapid temperature increase occurs a more precise definition of arises in the course of the development. In the present problem, during most of the time that t < tc, the material experiences only inert heat conduction because the heat-release term is exponentially small in the large parameter that measures E. The inert problem, with w = 0, has a known solution that can be derived by Laplace transforms, for example, and that can be written as... 

If f(t) = 0 for t < 0, then substitution of s = i into the above equation yields the definition of the Laplace transform. Thus, the Fourier transform is obtained from the Laplace transform solution (Equation 25) by the substitution s = i . The Fourier... 

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