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Function even

Figure 1. Numerical test of the reciprocal relations in Eqs. (9) anti (10) for Cg shown in Eq. (29), The values computeti directly from Eq. (29) are plotted upward and the values from the integral downward (by broken lines) for K/(ii= 16. The two curves are clearly identical, (a) ln C (/) against (//period). The modulus is an even function of /, (b) argC (f) against (//period). The phase is odd in /. Figure 1. Numerical test of the reciprocal relations in Eqs. (9) anti (10) for Cg shown in Eq. (29), The values computeti directly from Eq. (29) are plotted upward and the values from the integral downward (by broken lines) for K/(ii= 16. The two curves are clearly identical, (a) ln C (/) against (//period). The modulus is an even function of /, (b) argC (f) against (//period). The phase is odd in /.
A function for which/(re) = —f —x) over a specific intereval is called an odd function over that interval. If/(re) =f —x), the function is even. For example, y = jc, is an odd function over [—2,2]. The interval [—2,2] is symmetrical about X = 0. Write some odd functions. Write some even functions. Find a general rule for the integrals of odd functions over a symmetrical interval. Find a general rule for the integral of the product of an odd function and an even function over an inteiwal that is symmetrical for both. [Pg.30]

Next, for laminae orientations with 0 that are an even function of z (symmetric), as illustrated by the three-layered laminate in Figure 7-53b, the following integrands in b,d)> Equation (7.30), are odd ... [Pg.444]

Sinee the probability distribution functions (1) and (2) are even functions of Xia and Xg, respectively, the cross-term integral containing Xm and Xe to the first power will vanish.)... [Pg.6]

On introdueing (5) into (4), use is made of the fact that odd powers of aJm and x will always lead to zero integrals when multiplied by the even functions Pm and Pg. The different powers of x may thus be simply written as follows ... [Pg.7]

Tt2 are even functions of K, contours of touch any constant section of 712 at = 0, to give relative equilibria of the form... [Pg.74]

For A = 1, the eigenfunctions of IT are even functions of q, while for A = —1, they are odd functions of q. An even function of q is said to be of even parity, while odd parity refers to an odd function of q. Thus, the eigenfunctions of n are any well-behaved functions that are either of even or odd parity in their cartesian variables. [Pg.95]

We show next that the parity operator IT commutes with the Hamiltonian operator H if the potential energy F(q) is an even function of q. The kinetic energy term in the Hamiltonian operator is given by... [Pg.95]

If the potential energy of a system is an even function of the coordinates and if (q) is a solution of the time-independent Schrodinger equation, then the function is also a solution. When the eigenvalues of the Hamiltonian... [Pg.96]

Since E(x x) is an even function of x, this shows that... [Pg.33]

First of all, consider the parity of the integrands. In the first term onihe right-hand side of Eq. (39) both wavefunctions are either odd or even, thus their product is always even, while x3 is of course odd. The integral between symmetric limits of the resulting odd function of x vanishes and this term mates no contribution to the first-order perturbation. On the other hand the second term is different from zero, as x4 is an even function. [Pg.153]

In order for a transition to occur, the transition moment integral must be an even function. This integral is the product of the wave function corresponding to the ground state Tff, an operator R, and the wave function of the excited state Ye. Since R is antisymmetric, the product of the wave... [Pg.313]

If any one of these integrals (expectation value equations) is zero, the transition is said to be forbidden. For the electronic and spin wave functions, it is not necessary to evaluate the integral but only to note that an odd function integrated from minus infinity to infinity is zero, while an even function integrated within these limits results in a nonzero value. For example (Figure 2.1),... [Pg.317]

Only even functions of the linear case remain acceptable in the cyclic system and hence the quantum condition becomes L(= 27rr) = nX. The energy levels for a cyclic 7r-electron system follows immediately as... [Pg.328]

I ve had to learn to mask my symptoms to a point so that I can even function in the world. There is such a fine line between masking a little bit so it doesn t hurt your health, and masking so much that it does hurt your health. When I was going to bars, I masked way too much and it really hurt me. [Pg.83]

At its maxima, p must satisfy p" < 0, which suggests that such locations must lie within the classically allowed region. The same applies for the existence of inflection points in p. At the nodes of E, Equation 33.12 implies that p" > 0. At such points, p in fact has a minimum. Finally, when the potential is reflection symmetric then at the origin (x = 0), either E 0 (even function) or E 0 (odd function). For even... [Pg.525]

Changing x to — x in the first integral and recognizing that cos is an even function shows that b is zero for all n. The Fourier series expansion of the boxcar function is therefore... [Pg.102]


See other pages where Function even is mentioned: [Pg.184]    [Pg.133]    [Pg.119]    [Pg.26]    [Pg.90]    [Pg.443]    [Pg.443]    [Pg.308]    [Pg.333]    [Pg.154]    [Pg.63]    [Pg.63]    [Pg.360]    [Pg.96]    [Pg.237]    [Pg.322]    [Pg.883]    [Pg.34]    [Pg.143]    [Pg.161]    [Pg.173]    [Pg.205]    [Pg.219]    [Pg.18]    [Pg.382]    [Pg.295]    [Pg.237]    [Pg.79]    [Pg.318]    [Pg.140]    [Pg.41]    [Pg.106]   
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