Tag: Solutions
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Problem 2.8 – Griffith’s Intro to QM
Problem 2.8 A particle of mass m in the infinite square well (of width starts outin the state for some constant , so it is (at ) equally likely to be found at any point in the left half of the well. What is the probability that a measurement of the energy (at some later…
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Problem 2.7 – Griffith’s Intro to QM
Problem 2.7 A particle in the infinite square well has the initial wave function (a) Sketch , and determine the constant (b) Find .(c) What is the probability that a measurement of the energy would yield the value ?(d) Find the expectation value of the energy, using Equation 2.2. Solution: Peoblem 2.7 Solution (Download)
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Problem 2.6 – Griffith’s Intro to QM
Problem 2.6 Although the overall phase constant of the wave function is of no physical significance (it cancels out whenever you calculate a measurable quantity), the relative phase of the coefficients in Equation 2.17 does matter. For example, suppose we change the relative phase of and in Problem 2.5: where is some constant. Find ,…
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Problem 2.5 – Griffith’s Intro to QM
Problem 2.5 A particle in the infinite square well has as its initial wave function an even mixture of the first two stationary states: (a) Normalize . (That is, find This is very easy, if you exploit the orthonormality of and . Recall that, having normalized at , you can rest assured that it stays…
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Problem 2.4 – Griffith’s Intro to QM
Problem 2.4 Calculate , , , , , and , for the nth stationary state of the infinite square well. Check that the uncertainty principle is satisfied. Which state comes closest to the uncertainty limit? Solution: Problem 2.4 Solution (Download)
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Problem 2.3 – Griffith’s Intro to QM
Problem 2.3 Show that there is no acceptable solution to the (time-independent) Schrödinger equation for the infinite square well with or . (This is a special case of the general theorem in Problem 2.2, but this time do it by explicitly solving the Schrödinger equation, and showing that you cannot satisfy the boundary conditions.) Solution:…
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Problem 2.2 – Griffith’s Intro to QM
Problem 2.2 Show that must exceed the minimum value of , for every normalizable solution to the time-independent Schrödinger equation. What is the classical analog to this statement? Hint: Rewrite Equation 2.5 in the form if , then and its second derivative always have the same sign—argue that such a function cannot be normalized. Solution:…
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Problem 2.1 – Griffith’s Intro to QM
Problem 2.1 Prove the following three theorems: (a) For normalizable solutions, the separation constant must be real. Hint: Write (in Equation 2.7) as (with and real), and show that if Equation 1.20 is to hold for all , must be zero. (b) The time-independent wave function can always be taken to be real (unlike ,…
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Problem 7.9 (Schroeder’s Intro to Thermal Physics)
Problem 7.9 Compute the quantum volume for an molecule at room temperature, and argue that a gas of such molecules at atmospheric pressure can be treated using Boltzmann statistics. At about what temperature would quantum statistics become relevant for this system (keeping the density constant and pretending that the gas does not liquefy)? Solution: Problem…
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Problem 7.8 (Schroeder’s Intro to Thermal Physics)
Problem 7.8 Suppose you have a “box” in which each particle may occupy any of 10 single-particle states. For simplicity, assume that each of these states has energy zero. (a) What is the partition function of this system if the box contains only one particle? (b) What is the partition function of this system if…