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Euler identity

Note. In the proof above we have used the Euler identity... [Pg.433]

If the variations SV and SA could be substituted by the first-order differentials dV and dA, respectively, then the corresponding variation dil would become zero, in view of the equilibrium condition (18) and the Euler identity ... [Pg.386]

Trigonometric Functions. In modeling processes and in studying control systems, there are many other important time functions, such as the trigonometric functions, cos cor and sin cor, where co is the frequency in radians per unit time. The Laplace transform of cos cor or sin cor can be calculated using integration by parts. An alternative method is to use the Euler identity ... [Pg.43]

Another mathematically equivalent solution can be found by utilizing the following Euler identities (i = ) ... [Pg.7]

For example, the SHAKE algorithm [17] freezes out particular motions, such as bond stretching, using holonomic constraints. One of the differences between SHAKE and the present approach is that in SHAKE we have to know in advance the identity of the fast modes. No such restriction is imposed in the present investigation. Another related algorithm is the Backward Euler approach [18], in which a Langevin equation is solved and the slow modes are constantly cooled down. However, the Backward Euler scheme employs an initial value solver of the differential equation and therefore the increase in step size is limited. [Pg.272]

An identity due to Euler is important to know and is quite useful. It states that e = Cos0 + iSin0. [Pg.547]

To check the effect of integration, the following algorithms were tried Euler, explicit Runge-Kutta, semi-implicit and implicit Runge-Kutta with stepwise adjustment. All gave essentially identical results. In most cases, equations do not get stiff before the onset of temperature runaway. Above that, results are not interesting since tubular reactors should not be... [Pg.168]

We now repeat the problem with the s = jco substitution in the characteristic equation, and rewrite the time delay function with Euler s identity ... [Pg.132]

Apply Euler s identity and the final result for the normalized response is V (t)l... [Pg.144]

P(Qol, t) is the conditional probability of the orientation being at time t, provided it was Qq a t time zero. The symbol — F is the rotational diffusion operator. In the simplest possible case, F then takes the form of the Laplace operator, acting on the Euler angles ( ml) specifying the orientation of the molecule-fixed frame with respect to the laboratory frame, multiplied with a rotational diffusion coefficient. Dr. Equation (44) then becomes identical to the isotropic rotational diffusion equation. The rotational diffusion coefficient is simply related to the rotational correlation time introduced earlier, by tr = 1I6Dr. [Pg.65]

The 1/r solution is in fact just an Euler s method approximation to the integral for the PFTR, in which one approximates the integral as a summation. The calculation is not very accurate because we used a 0.2 moles/liter step size to keep the spreadsheet small, but it illustrates the method and the identity between Euler s method and a spreadsheet solution. [Pg.228]

Hydrodynamic dimensionless numbers Examples are the Reynolds number, Froude, Archimedes, and Euler number. These dimensionless numbers have to be functions of identical determining dimensionless numbers of the same powers and with the same value of the other constant coefficients, so that the model and the object are similar. [Pg.525]

Therefore the fact that 9 is arbitrary in U(l) theory compels that theory to assert that photon mass is zero. This is an unphysical result based on the Lorentz group. When we come to consider the Poincare group, as in section XIII, we find that the Wigner little group for a particle with identically zero mass is E(2), and this is unphysical. Since 9 in the U(l) gauge transform is entirely arbitrary, it is also unphysical. On the U(l) level, the Euler-Lagrange equation (825) seems to contain four unknowns, the four components of , and the field tensor H v seems to contain six unknowns. This situation is simply the result of the term 7/MV in the initial Lagrangian (824) from which Eq. (826) is obtained. However, the fundamental field tensor is defined by the 4-curl ... [Pg.242]

This same qualitative difference between adrenaline and noradrenaline obtains for the splenic artery/splenic vein equipressor dosage-response ratios as well, and both observations quite possibly may find their explanation in the recent work of Euler (64-70). He has found that the pressor substance isolated from the heart, blood, liver, and spleen has predominantly the characteristics of noradrenaline. Thus, he has considered Sympathin E to be identical with Z-noradrenaline. [Pg.41]

Scalar counting relations for sets of structural components can seen as expressions for characters under the identity operation of more general relations between representations of those sets. For example, the Euler relation in topology can be generalised to connect not only the numbers of edges, vertices and faces of a polyhedron, but also various symmetries associated with the structural features. The well-known Euler theorem... [Pg.225]


See other pages where Euler identity is mentioned: [Pg.561]    [Pg.393]    [Pg.83]    [Pg.42]    [Pg.271]    [Pg.15]    [Pg.257]    [Pg.509]    [Pg.130]    [Pg.561]    [Pg.393]    [Pg.83]    [Pg.42]    [Pg.271]    [Pg.15]    [Pg.257]    [Pg.509]    [Pg.130]    [Pg.181]    [Pg.1183]    [Pg.661]    [Pg.429]    [Pg.66]    [Pg.9]    [Pg.9]    [Pg.485]    [Pg.96]    [Pg.21]    [Pg.792]    [Pg.240]    [Pg.116]    [Pg.128]    [Pg.12]    [Pg.255]    [Pg.135]    [Pg.459]    [Pg.76]    [Pg.125]    [Pg.126]    [Pg.97]   
See also in sourсe #XX -- [ Pg.393 ]




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Euler’s identity

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