Why can’t you do integration-by-parts directly on the middle expression in Equation -1.29 pull the time derivative over onto x, note thatx/t=0 , and conclude thatd<x>/dt=0 ?

Short Answer

Expert verified

Because the derivative and integrals are taken with respect to different variables t and x,so the integration-by-parts is not possible.

Step by step solution

01

The given information

The equation 1.29 is,

dxdt=xtΨ2dx=ih2mxtΨ*Ψt-Ψ*tΨdx

According to the given question, X/T=0. Integration-by-parts directly cannot be done on the middle expression dxdt=xtΨ2dx=ih2mxtΨ*Ψt-Ψ*tΨdx.

02

The expected equation and the variables.

The expected value is the average of the results of a large number of measurements taken on separate systems.

The following is the expression for X's expected value:

X=Ψ*x,txΨx,tdxX=xΨx,t2dx

The wave function is Ψx,t, and the average value or expectation value of the position operator x is x.

03

The differentiate of the equation and put the value of  x

The above equation have to be differentiated on both sides:

dxdt=xtΨ2dx

The time derivative will be put on to xas the condition is given. So, the equation is:

dxdt=xtxΨ2dx=tΨ2dx+xtΨ2dx=0+xtΨ2dx=xtΨ2dx

04

The limit of the equation

Taking the above equation in between aand b,the equation will be:

dxdt=batxΨ2dx=xΨ2dxab

The derivative is with regard to time, while the integration is with respect toxin the above integration.

As a result, part-by-part integration is not possible.

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Most popular questions from this chapter

For the distribution of ages in the example in Section 1.3.1:

(a) Computej2 andj2 .

(b) Determine ∆j for each j, and use Equation 1.11 to compute the standard deviation.

(c) Use your results in (a) and (b) to check Equation 1.12.

Suppose you wanted to describe an unstable particle, that spontaneously disintegrates with a lifetime in that case the total probability of finding the particle somewhere should not be constant but should decrease at an exponential rate:

p(t)=-[ψx,t2]dx=e-tt

A crude way of achieving this result is as follows. in equation 1.24 we tightly assumed that is real. That is certainly responsible, but it leads to the conservation of probability enshrined in equation 1.27. What if we assign to in imaginary part

V=V0=iΓ

Where is the true potential energy and is a positive real constant?

  1. Show that now we get

dpdt=2Γhp.

Solve for and find the lifetime of the particle in terms ofΓ

Consider the first 25 digits in the decimal expansion of π (3, 1, 4, 1, 5, 9, . . .).

(a) If you selected one number at random, from this set, what are the probabilities of getting each of the 10 digits?

(b) What is the most probable digit? What is the median digit? What is the average value?

(c) Find the standard deviation for this distribution.

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ψ(x,t)=Ae-λ|x|e-iωt

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(a) Normalizeψ .

(b) Determine the expectation values ofx and x2.

(c) Find the standard deviation of . Sketch the graph ofΨ2 , as a function ofx, and mark the points (x+σ)and (x-σ), to illustrate the sense in whichσ represents the “spread” inx. What is the probability that the particle would be found outside this range?

Consider the Gaussian distribution

ρ(x)=Aeλ(xa)2

where A, a, and λ are positive real constants. (Look up any integrals you need.)

(a) Use Equation 1.16 to determine A.

(b) Find〈x〉,〈x2〉,and σ.

(c) Sketch the graph of ρ(x).

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