Chap35 - 35.1 QUANTUM MECHANICS EXERCISES Section 35.2 The Schrödinger Equation 10 The one-dimensional wave function is related to the probability

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Unformatted text preview: 35.1 QUANTUM MECHANICS EXERCISES Section 35.2 The Schrödinger Equation 10. The one-dimensional wave function is related to the probability by Equation 35.2, 2 ( ) . dP x dx ψ = Since probability (a pure number) is dimensionless, the units of ψ must be the square root of the inverse of the units of x (a length), or 1/ 2 (meters) . − 11. INTERPRET We are given the wave function of a particle and asked about its probability distribution. DEVELOP Since the quantity 2 ( ) x ψ represents the probability density of finding the particle, the particle is most likely to be found at the position where the probability density 2 ( ) x ψ is a maximum. EVALUATE (a) The maximum of 2 2 2 2 2 / ( ) x a x A e ψ − = is at x = (calculate 2 ( )/ d dx ψ = for corroboration). (b) The probability density 2 ( ) x ψ falls to half its maximum value 2 2 ( (0) ) A ψ = when 2 2 2 / 1/2 , x a e − = or 1 2 ln2 0.589 . x a a = ± = ± ASSESS The probability distribution is shown below. Note that 2 2 2 2 2 / ( )/ x a x A e ψ − = peaks at x = and is halved at / 0.589. x a = ± 12. INTERPRET We normalize the wave function that is given graphically in Figure 35.19. The particle must be somewhere , so the normalization constant is chosen such that the integral of the wave function over all space is one. DEVELOP The probability of finding the particle within dx of x is 2 ( ) ( ). P x x ψ = We will write an equation for the wave function, square it, and integrate. Then we’ll set the value of A such that the integral over the entire region is one. EVALUATE For 2 , L x ≤ ≤ 2 ( ) . A L x x ψ = Since the wave function is symmetric, we’ll just integrate from x = to 2 L x = and multiply by 2 to obtain the integral over all space. 3 2 2 2 2 / 2 2 2 4 3 1 2 3 3 L A x A L A L dx A L L L = = = → = ∫ ASSESS The actual wave function for the region 2 L x ≤ ≤ is then 3/ 2 2 3 ( ) . L x x ψ = 13. INTERPRET We use the normalization constant and the wave function from Exercise 12 to find the probability of finding the particle in the region 4 . L x ≤ ≤ The probability of finding a particle in a region dx is 2 . dx Ψ DEVELOP We integrate the square of the normalized wave function 3/ 2 2 3 ( ) L x x ψ = from x = to 4 L x = to find the probability of finding the particle in the region 4 . L x ≤ ≤ 35 35.2 Chapter 35 EVALUATE 3 / 4 2 3 3 3 12 12 1 1 3 16 4 L L P x dx L L = = = ∫ ASSESS There is a one in sixteen chance of finding the particle in the region described. The region is a quarter of the entire region where the particle could be, but the wave function is smaller in this region than elsewhere so the probability is less than one in four....
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This note was uploaded on 10/21/2010 for the course PHYSICS 2131441 taught by Professor Pheong during the Fall '10 term at University of California, Berkeley.

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Chap35 - 35.1 QUANTUM MECHANICS EXERCISES Section 35.2 The Schrödinger Equation 10 The one-dimensional wave function is related to the probability

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