Difference between the average position and the most likely position of a particle

In summary, The two parts (a) and (b) are not the same, as they are asking for different values of the particle's position. Part (a) is asking for the average position, which can be calculated by finding the area under the probability distribution curve. Part (b) is asking for the most likely position, which can be found by locating the maximum of the probability distribution curve. In order to solve these problems, integration by parts can be used to evaluate the integrals.
  • #71


yes that is true, the wave functions are, in general, complex valued. However, their modulus square is real :-)
 
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  • #72


Okay so if we insert in B:

[tex] = -(2\beta)^2x2 \beta e^{-2\beta x} + (2\beta)^2e^{-2\beta x} [/tex]

[tex] = -8x\beta^3 e^{-2\beta x} + 4\beta^2e^{-2\beta x} [/tex]

So does this look okay?
 
  • #73


yes, then what is the value of x which gives the derivative equal to zero?
 
  • #74


It is going to be infinity, because both sides have e^-x, and only one has x before hand, so we need the e^-x = 0, which means x must be infinity
 
  • #75


no no no no no

[tex]
0 = -8x\beta^3 e^{-2\beta x} + 4\beta^2e^{-2\beta x}
[/tex]

Show me how you solve it.
 
  • #76


[itex]x \to \infty[/itex] is one extremum, but certainly not a maximum...[itex]P(x \to \infty)=0[/itex]...There is one more solution to that equation which does correspond to a maximum.
 
  • #77


Well, you want x on one side, so:

[tex] 0 = -8x\beta^3 e^{-2\beta x} + 4\beta^2e^{-2\beta x} [/tex]

[tex] 8x\beta^3 e^{-2\beta x} = 4\beta^2e^{-2\beta x} [/tex]

[tex] 2x\beta^3 e^{-2\beta x} = \beta^2e^{-2\beta x} [/tex]

[tex] 2x e^{-2\beta x} = \frac{\beta^2}{\beta^3}e^{-2\beta x} [/tex]

[tex] 2x e^{-2\beta x} = \beta^{-2}e^{-2\beta x} [/tex]

[tex] 2x = \beta^{-2}\frac{e^{-2\beta x}}{e^{-2\beta x}} [/tex]

[tex] 2x = \beta^{-2} [/tex]

[tex] x = \frac{\beta^{-2}}{2} [/tex]

How is this?
 
  • #78


[tex]
2x e^{-2\beta x} = \frac{\beta^2}{\beta^3}e^{-2\beta x}
[/tex]

is not

[tex]
2x e^{-2\beta x} = \beta^{-2}e^{-2\beta x}
[/tex]

(I am faster than gabbagabbahey ! :-D )
 
  • #79


[tex]\frac{\beta^2}{\beta^3}=\frac{1}{\beta}\neq\beta^{-2}[/tex] :wink:
 
  • #80


Hmm, why did I do that?

[tex] 2x e^{-2\beta x} = \beta^{-1}e^{-2\beta x} [/tex]

[tex] 2x = \beta^{-1}\frac{e^{-2\beta x}}{e^{-2\beta x}} [/tex]

[tex] 2x = \beta^{-1} [/tex]

[tex] x = \frac{\beta^{-1}}{2} [/tex]

Is this better?
 
  • #81


yes! :-)

or nicer [tex]
x = \frac{1}{2\beta}
[/tex]
 
  • #82


Don't forget to express [itex]\langle x \rangle[/itex] in terms of [itex]\beta[/itex] in order to properly compare the average value to the expected value :smile:
 
  • #83


Okay so:

Average Position:

[tex] \frac{4\beta^2}{4\beta^3}\right] [/tex]

[tex] \frac{1}{\beta}\right] [/tex]

And the Most probable position:

[tex] \frac{1}{2\beta} [/tex]
 
  • #84


yup, quite cool isn't it?

the reason for this is that the wave function has a long 'tail' which makes more 'probability' lie to the right of its maximum (c.f Maxwell speed distribution)
 
  • #85


Indeed, not much difference, just *half more

Would the Standard deviation for this be the difference, or will I need to use:

[tex] |Delta x = \sqrt{<x^2> - <x>^2} [\tex]
 
  • #86


you have to use it
 
  • #87


Okay so:

[tex] <x^2> = \int^{\infty}_0 x^2 P(x) [/tex]

P(x) = B^2 x e^{-2\beta x}

[tex] <x^2> = \int^{\infty}_0 x^2B^2 x e^{-2\beta x} [/tex]

[tex] <x^2> = \int^{\infty}_0 x^3B^2 e^{-2\beta x} [/tex]

[tex] <x^2> = B^2 \int^{\infty}_0 x^3e^{-2\beta x} [/tex]

I have a feeling that this integral will have to be done three times...

Okay so first time:

[tex] \left[\int^{\infty}_0 x^3e^{-2\beta x}\right] [/tex]

[tex] f(x) = x^3, f'(x) = 3x^2 [/tex]

[tex] g'(x) = e^{-2\beta x}, g(x) = -\frac{1}{2\beta}e^{-2\beta x} [/tex]

Thus:

[tex] \left[ -x^3\frac{1}{2\beta}e^{-2\beta x} - \int -3x^2\frac{1}{2\beta}e^{-2\beta x} \right] [/tex]

[tex] \left[ -x^3\frac{1}{2\beta}e^{-2\beta x} + \frac{3}{2\beta}\int x^2e^{-2\beta x} \right] [/tex]

Okay so far?
 
  • #88


so now you added a question to the original one, how rude!

and I/we don't have to feed you like a baby, have some confident
[tex]
\int x^2e^{-2\beta x} \, dx
[/tex]
now you know what the integral is, you did earlier
 
  • #89


Sorry
 
  • #90


how's it going?
 
  • #91


OKay, well I have:

[tex] B^2\left[ -\frac{1}{2\beta}e^{-2\beta x} + frac{3}{2 \beta\left[ -frac{-x^2}{2\beta}e^{-2 \beta x} + \frac{1}{\beta} \left[ \frac{x}{2\beta}e^{-2\beta x} + 1\frac{1}{2\beta} \left[ -\frac{1}{2\beta} e^{-2\beta x} \right]\right] /right]} \right] [/tex]

Which I have reduced to:

[tex] B^2\left[-\frac{x^3}{2\beta}e^{-2\beta x} + \frac(-\frac{3x^2}{4\beta^2}e^{-2\beta x} + \frac{3x}{4\beta^3}e^{-2\beta x} - \frac{3}{8\beta^4}e^{-2 \beta x} \right] [/tex]

[tex] B^2 = 4\beta^2[/tex]

[tex] \left[-\frac{B^2x^3}{2\beta}e^{-2\beta x} - \frac{B^23x^2}{4\beta^2}e^{-2\beta x} + \frac{B^23x}{4\beta^3}e^{-2\beta x} - \frac{3B^2}{8\beta^4}e^{-2 \beta x} \right] [/tex]

[tex] \left[-\frac{4\beta x^3}{2}e^{-2\beta x} - 3x^2e^{-2\beta x} + \frac{3x}{4\beta}e^{-2\beta x} - \frac{3}{2\beta^2}e^{-2 \beta x} \right] [/tex]
 
  • #92

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