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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.

Short Answer

Expert verified
  1. Probability of choosing each digit is shown in the solution.
  2. Most probable digit = 3, Median digit = 4, Average value = 28.4.
  3. σ=2.47

Step by step solution

01

Solution:

First 25 decimal digits of π is,

π=3.141592653589793238462643...

02

Finding the probability of choosing a particular digit

Part (a)

The probability of choosing a particular digit is the frequency, divided by the total number of digits

0:025=05:325=0.121:225=0.086:325=0.122:325=0.127:125=0.043:525=0.208:225=0.084:325=0.129:325=0.12

03

Write the set of all the numbers from smallest to largest

Part (b)

{1,1,2,2,2,3,3,3,3,3,4,4,4,5,5,5,6,6,6,7,8,8,9,9,9}

The highlighted number in this set represents the median

Median = 4

Most probable digit chosen is 3 since it’s the number with highest frequency

04

Calculating the average value

The average value is given by the expectation value.

j=jjNjjNjj=0*0+1*2+2*3+3*5+4*3+5*3+6*3+7*1+8*2+9*30+2+3+5+3+3+3+1+2+3j=71025j=28.4

Thus, the most probable digit, median, and average value are 4, 3, and 28.4 respectively.

05

Calculating the standard deviation

Standard deviation is given by

σ=j2j2σ=28.44.722σ=2.47

Thus, the standard deviation is 2.47.

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Most popular questions from this chapter

In general, quantum mechanics is relevant when the de Broglie wavelength of the principle in question(h/p) is greater than the characteristic Size of the system (d). in thermal equilibrium at (kelvin) TemperatureT the average kinetic energy of a particle is

p22m=32kBT

(Where kBis Boltzmann's constant), so the typical de Broglie wavelength is

λ=h3mkBT.

The purpose of this problem is to anticipate which systems will have to be treated quantum mechanically, and which can safely be described classically.

(a) Solids. The lattice spacing in a typical solid is aroundd=0.3nm . Find the temperature below which the free 18electrons in a solid are quantum mechanical. Below what temperature are the nuclei in a solid quantum mechanical? (Use sodium as a typical case.) Moral: The free electrons in a solid are always quantum mechanical; the nuclei are almost never quantum mechanical. The same goes for liquids (for which the interatonic spacing is roughly the same), with the exception of helium below4K .

(b) Gases. For what temperatures are the atoms in an ideal gas at pressure quantum mechanical? Hint: Use the ideal gas law (PV=NkBT)to deduce the interatomic spacing.

Question: Let pab(t)be the probability of finding a particle in the range (a<x<b),at time t.

(a)Show that

dpabdt=j(a.t)-j(b,t),

Where

j(x,t)ih2m(ψψ*x-ψ*ψx)

What are the units of j(x,t)?

Comment: j is called the probability current, because it tells you the rate at which probability is "flowing" past the point x. Ifpab(t) is increasing, then more probability is flowing into the region at one end than flows out at the other.

(b) Find the probability current for the wave function in Problem 1.9. (This is not a very pithy example, I'm afraid; we'll encounter more substantial ones in due course.)

The needle on a broken car speedometer is free to swing, and bounces perfectly off the pins at either end, so that if you give it a flick it is equally likely to come to rest at any angle between 0 tox.

  1. What is the probability density? Hint: ρ(θ)dθ is the probability that the needle will come to rest betweenθ andθ+dθ .
  2. Computeθ ,θ2 , andσ , for this distribution.
  3. Computesinθ ,cosθ , andcos2θ

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 ?

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