Docsity
Docsity

Prepare for your exams
Prepare for your exams

Study with the several resources on Docsity


Earn points to download
Earn points to download

Earn points by helping other students or get them with a premium plan


Guidelines and tips
Guidelines and tips

Solutions to Homework 1 - Quantum Mechanics | PHYS 324, Assignments of Quantum Mechanics

Material Type: Assignment; Class: QUANTUM MECHANICS; Subject: Physics; University: University of Washington - Seattle; Term: Unknown 1989;

Typology: Assignments

Pre 2010

Uploaded on 03/10/2009

koofers-user-0hf-1
koofers-user-0hf-1 🇺🇸

5

(1)

10 documents

1 / 2

Toggle sidebar

Related documents


Partial preview of the text

Download Solutions to Homework 1 - Quantum Mechanics | PHYS 324 and more Assignments Quantum Mechanics in PDF only on Docsity! Solution to Homework Set # 1 1. λ = h/p and p2/2m = KE = 3kBT/2. Therefore: p = √ 3mkBT = √ 3 × 1.67× 10−27kg × 1.38× 10−23J/K × 300K = 4.55× 10−24kg −m/s Then, λ = (6.626× 10−34J s)/(4.55× 10−24kg −m/s) = 1.46× 10−10 m. Note, this wavelength is comparable to the spacing between atoms in a solid, making thermal neutron beams a useful tool for studying the structure of materials. 2. (Problem 1.7 in the text) (a) ∫ ∞ −∞ ψ(x, 0) ∗ψ(x, 0)dx = 1 = A2 [ ∫ a 0 (x/a) 2dx + ∫ b a (b− x) 2/(b− a)2dx ] Changing variables to y = b− x in the second integral, 1 = A2 [ x3 3a2 ∣∣∣ a 0 + y3 3(b− a)2 ∣∣∣ b−a 0 ] = A2 [a 3 + b− a 3 ] = A2 × b 3 Therefore, A = √ 3/b. (b) ψ(x, 0) starts at 0 when x = 0 and increases linearly to a value of A when x = a. It then decreases linearly from a value of A at x = a to 0 when x = b. (c) The particle is most likely to be found where ψ(x, 0)∗ψ(x, 0) is largest because |ψ(x)|2 is the prob- ability density for finding the particle at x. From part (b), you see that ψ(x, 0)∗ψ(x, 0) is largest at x = a where it takes the value of A2 = 3/b. Therefore, at t = 0, the particle is most likely to found near x = a. (d) If P (x) is a probability density, then the probability of finding x to be between a and b is given by∫ b a P (x)dx. The probability of finding our particle to the left of a is then: P (x < a) = ∫ a −∞ ψ(x, 0)∗ψ(x, 0)dx = A2 ∫ a 0 (x/a)2dx = A2 x3 3a2 ∣∣∣ a 0 = 3 b × a 3 = a b When b = a, P (x < a) = 1 as it should because ψ(x, 0) = 0 for x > b. When b = 2a, ψ(x, 0) is symmetric about x = a, so we expect P (x < a) to be 1/2, in agreement with our result. (e) 〈x(t = 0)〉 = ∫ ∞ −∞ ψ(x, 0) ∗ x ψ(x, 0) dx: 〈x(t = 0)〉 = A2 [ ∫ a 0 x3 a2 dx + ∫ b a x(b− x)2 (b− a)2 dx ] = 3 b [ x4 4a2 ∣∣∣ a 0 + b2x2/2 − 2bx3/3 + x4/4 (b− a)2 ∣∣∣ b a ] = 3 b [a2 4 + 1 (b− a)2 [b2(b2 − a2) 2 − 2b(b 3 − a3) 3 + b4 − a4 4 ]] = 3 b [a2 4 + 1 12(b− a)2 [ b4 − 6b2a2 + 8ba3 − 3a4 ]] = 3 b [a2 4 + 1 12(b− a)2 [ (b− a)2(b2 + 2ba− 3a2) ]] = 3 b [a2 4 + b2 + 2ba 12 − a 2 4 ] = b+ 2a 4 1
Docsity logo



Copyright © 2024 Ladybird Srl - Via Leonardo da Vinci 16, 10126, Torino, Italy - VAT 10816460017 - All rights reserved