1 x 2!, (21) or in shorthand x˙ = Jx, (22) where J is the so-called Jacobian matrix, whose entries are the partial derivatives of the right hand sides of the differential equations describing the model, taken with respect to the different state variables of the model (e.g. S and I). We often write the entries of J as
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بیشترP2 2m + 1 2 m!2X2 ‚ jˆ> = E n jˆ> : Postscript: Notice that this Schrodinger equation is basis independent. The momentum and position operators are represented only in abstract Hilbert space. 2. Show that the time-independent Schrodinger Equation for the SHO can be written „h! µ aya+ 1 2 ¶ jˆ> = E n jˆ> : Let a = µ m! 2„h ¶ 1=2 X ...
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بیشتر2. sinasinb= 1 2 [cos(a b) cos(a+ b)]. See the comment after Exercise 7, H4.4. Problem XC-H4.4-9. (Energy Conservation) From u tt= c2u xx, derive conservation of energy for a vibrating string, dE dt = c2 u x(x;t)u t(x;t)j x=L x=0; where the total energy Eis the sum of the kinetic energy, de ned by R L 0 1 2 (u t) 2dx, and the potential energy ...
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