Drawing conclusions by looking at integral

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Homework Help Overview

The discussion revolves around evaluating the integral expression involving normalized distributions, specifically focusing on the conditions under which the integral may be positive. The integral is defined over two intervals, one from negative infinity to zero and the other from zero to positive infinity, with the distributions exhibiting specific symmetry properties.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the possibility of expressing one part of the integral in terms of the other, questioning the assumptions about symmetry in the distributions. There are discussions about potential counterexamples where the integral could yield different signs based on the properties of the functions involved.

Discussion Status

Participants are actively engaging with the problem, offering various approaches and questioning the validity of assumptions. Some have suggested specific cases and counterexamples that could challenge the initial hypothesis about the positivity of the integral, indicating a productive exploration of the topic.

Contextual Notes

There is an ongoing examination of the implications of symmetry in the distributions and the potential for different outcomes based on the specific forms of the functions involved. Participants are also considering the limitations of using certain mathematical constructs, such as the Dirac delta function, in their arguments.

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Homework Statement



I have the following expression

$$I = \int_{-\infty}^{0} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp + \int_{0}^{\infty} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp$$

where ##f_p## and ##f_x## are normalised distributions. In particular, ##f_x## is symmetric about ##x=a##. This also means that ##pf_x(a - \frac{p}{m}t) ## is anti-symmetric about ##p = 0##.

Is there any way through which I can prove (or disprove) that ##I## is positive if
$$\int_{-\infty}^{0} f_p(p) dp < \int_{0}^{\infty} f_p(p) dp $$
ie the area under the graph on the -ve ##p##-axis is smaller than that on the +ve ##p##-axis?

Some guidance regarding how to start is greatly appreciated. Thanks in advance!

Homework Equations

The Attempt at a Solution

 
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I would try to express the (negative) left side wrt the (positive) side. I.E. something like - (int_0^+inf, the integrand will change but you have properties of f and f_x to help you out. PLEASE, let me know if/how that helps.

(Dr.) Dave
 
Can't you come up with a counterexample where ##f_p(p)## and ##g_p(p) = pf_x(a-\frac pm t)## don't overlap so that ##I=0##?
 
Thank you both for replying!

To Dr Dave:
David Dyer said:
I would try to express the (negative) left side wrt the (positive) side. I.E. something like - (int_0^+inf, the integrand will change but you have properties of f and f_x to help you out. PLEASE, let me know if/how that helps.
hmm, does this not assume that ##f_p## is symmetric about 0 as well? I'm not sure I'm allowed to make such an assumption in my problem if that is the case.

To vela:
vela said:
Can't you come up with a counterexample where ##f_p(p)## and ##g_p(p) = pf_x(a-\frac pm t)## don't overlap so that ##I=0##?
So if I have ##g_p (p)## that asymptotes at about ##p = \pm 5## ,and I have a ##f_p## that has gaussian peaks at ##p = -1## (area of ~ 0.4) and ##p = 20## (area of ~0.6), I can even have a negative value for ##I## despite ##\int_{-\infty}^{0} f_p(p) dp < \int_{0}^{\infty} f_p(p) dp##

Is this right?
 
WWCY said:

Homework Statement



I have the following expression

$$I = \int_{-\infty}^{0} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp + \int_{0}^{\infty} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp$$

where ##f_p## and ##f_x## are normalised distributions. In particular, ##f_x## is symmetric about ##x=a##. This also means that ##pf_x(a - \frac{p}{m}t) ## is anti-symmetric about ##p = 0##.

Is there any way through which I can prove (or disprove) that ##I## is positive if
$$\int_{-\infty}^{0} f_p(p) dp < \int_{0}^{\infty} f_p(p) dp $$
ie the area under the graph on the -ve ##p##-axis is smaller than that on the +ve ##p##-axis?

Some guidance regarding how to start is greatly appreciated. Thanks in advance!

Homework Equations

The Attempt at a Solution


Let ##I = I_1 +I_2,## where ##I_1## is the first integral and ##I_2## is the second one. Putting ##p = -p'## in ##I_2## we have
$$I_2 = \int_{\infty}^0 f_p(-p') (-p') f_x\left(a + \frac{p'}{m}t \right) (-dp')\\ = -\int_0^{\infty} f_p(-p') p' f_x\left(a +\frac{p'}{m}t \right) \, dp'.$$
Now change the integration variable back to ##p## and use symmetry of ##f_x##, to get
$$I = \int_0^{\infty} p [f_p(p)-f_p(-p)] f_x\left(a - \frac{p}{m} t \right) \, dp.$$
 
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Ray Vickson said:
Let ##I = I_1 +I_2,## where ##I_1## is the first integral and ##I_2## is the second one. Putting ##p = -p'## in ##I_2## we have
$$I_2 = \int_{\infty}^0 f_p(-p') (-p') f_x\left(a + \frac{p'}{m}t \right) (-dp')\\ = -\int_0^{\infty} f_p(-p') p' f_x\left(a +\frac{p'}{m}t \right) \, dp'.$$
Now change the integration variable back to ##p## and use symmetry of ##f_x##, to get
$$I = \int_0^{\infty} p [f_p(p)-f_p(-p)] f_x\left(a - \frac{p}{m} t \right) \, dp.$$

Thank you so much for helping out!

Edit: Does this apply to ##I_1## instead of ##I_2##? I'm am not really able to see why the integration limits for ##I_2## carry the same sign despite the change in variables.
 
WWCY said:

Homework Statement



I have the following expression

$$I = \int_{-\infty}^{0} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp + \int_{0}^{\infty} f_p(p) \ \big[ pf_x(a - \frac{p}{m}t) \big] dp$$

where ##f_p## and ##f_x## are normalised distributions. In particular, ##f_x## is symmetric about ##x=a##. This also means that ##pf_x(a - \frac{p}{m}t) ## is anti-symmetric about ##p = 0##.

Is there any way through which I can prove (or disprove) that ##I## is positive if
$$\int_{-\infty}^{0} f_p(p) dp < \int_{0}^{\infty} f_p(p) dp $$
ie the area under the graph on the -ve ##p##-axis is smaller than that on the +ve ##p##-axis?

Some guidance regarding how to start is greatly appreciated. Thanks in advance!

Homework Equations

The Attempt at a Solution

I think the result is incorrect.

First note that you can write your integral ##I## as
$$I = \int_{-\infty}^{\infty} p f_p(p) f_x\left(a- \frac{pt}{m} \right) \, dp$$
Now consider a special case of
$$f_x(w) = \frac{1}{2} \delta(w+b) + \frac{1}{2} \delta(w-b),$$
where ##\delta(u) ## is the Dirac delta-function and ##b > 0##. The delta-function is even, so ##f_x## is also even in ##w##.

Now we get
$$I = \frac{m^2}{2 t^2} \left[(a+b)f_p\left(\frac{m(a+b)}{t} \right) +(a-b) f_p\left(\frac{m(a-b)}{t} \right) \right] \hspace{5ex}(1)$$
By playing with the function ##f_p## and the value of ##b## it will be possible to have ##I < 0## in some cases, but ##I > 0## in other cases.

Of course, you could object that the Dirac delta is not a true, "legitimate" function, but it IS a limit of a sequence of true functions, and so there are true functions that essentially mimic eq. (1), and so give counterexamples to what you hoped.
 
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Ray Vickson said:
I think the result is incorrect.

First note that you can write your integral ##I## as
$$I = \int_{-\infty}^{\infty} p f_p(p) f_x\left(a- \frac{pt}{m} \right) \, dp$$
Now consider a special case of
$$f_x(w) = \frac{1}{2} \delta(w+b) + \frac{1}{2} \delta(w-b),$$
where ##\delta(u) ## is the Dirac delta-function and ##b > 0##. The delta-function is even, so ##f_x## is also even in ##w##.

Now we get
$$I = \frac{m^2}{2 t^2} \left[(a+b)f_p\left(\frac{m(a+b)}{t} \right) +(a-b) f_p\left(\frac{m(a-b)}{t} \right) \right] \hspace{5ex}(1)$$
By playing with the function ##f_p## and the value of ##b## it will be possible to have ##I < 0## in some cases, but ##I > 0## in other cases.

Of course, you could object that the Dirac delta is not a true, "legitimate" function, but it IS a limit of a sequence of true functions, and so there are true functions that essentially mimic eq. (1), and so give counterexamples to what you hoped.

I believe I see it clearly now, many thanks for your assistance!
 

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