Solution for complex differentiation and integration.

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Following my question here, I am able to solve up to a point beyond which I would really appreciate any help (also if my current understanding is right).



Note that I have to find $f_T(t)$. The question starts with:



$$P(T<t) = 1-int_mathcalVexp(-lambdapi v^2t^2)dP_V(v).$$



with $T, V$ are random variables with values $t,v$ denoting time and speed. $mathcalV$ is the range of $V$. $lambda$ is a rate (constant).
The final answer should be:



$$f_T(t) = fracg(v_min) - g(v_max)(v_max - v_min)t, tgeq0$$
where $$g(x) = xe^-lambda pi t^2x^2 + frac1sqrtlambdatQ(sqrt2pilambda t x)$$ and $$Q(x) = frac1sqrt2piint_x^infty e^fracu^22du$$




My Solution



Let velocity be a continous uniform distribution with range $[v_min,v_max] = [v_0,v_1]$, so above eq. would become:



$$P(T<t) = 1-int_v_0^v_1exp(-lambdapi v^2t^2)Big(frac1v_1-v_0Big)dv.$$



$$f_T(t) = -Big(frac1v_1-v_0Big)fracddtint_v_0^v_1exp(-lambdapi v^2t^2) dv.$$



using the property $int e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[texterf(sqrtpilambda tv_1) - texterf(sqrtpilambda tv_0)].$$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[Q(sqrtpilambda tv_0) - Q(sqrtpilambda tv_1)].$$



I cannot reach beyond this point. Any help would be much appreciated.







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  • I am not familiar with random variables. Are you actually stuck at the point of differentiation?
    – Szeto
    Aug 1 at 2:05










  • Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
    – Kashan
    Aug 1 at 3:04














up vote
0
down vote

favorite
1












Following my question here, I am able to solve up to a point beyond which I would really appreciate any help (also if my current understanding is right).



Note that I have to find $f_T(t)$. The question starts with:



$$P(T<t) = 1-int_mathcalVexp(-lambdapi v^2t^2)dP_V(v).$$



with $T, V$ are random variables with values $t,v$ denoting time and speed. $mathcalV$ is the range of $V$. $lambda$ is a rate (constant).
The final answer should be:



$$f_T(t) = fracg(v_min) - g(v_max)(v_max - v_min)t, tgeq0$$
where $$g(x) = xe^-lambda pi t^2x^2 + frac1sqrtlambdatQ(sqrt2pilambda t x)$$ and $$Q(x) = frac1sqrt2piint_x^infty e^fracu^22du$$




My Solution



Let velocity be a continous uniform distribution with range $[v_min,v_max] = [v_0,v_1]$, so above eq. would become:



$$P(T<t) = 1-int_v_0^v_1exp(-lambdapi v^2t^2)Big(frac1v_1-v_0Big)dv.$$



$$f_T(t) = -Big(frac1v_1-v_0Big)fracddtint_v_0^v_1exp(-lambdapi v^2t^2) dv.$$



using the property $int e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[texterf(sqrtpilambda tv_1) - texterf(sqrtpilambda tv_0)].$$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[Q(sqrtpilambda tv_0) - Q(sqrtpilambda tv_1)].$$



I cannot reach beyond this point. Any help would be much appreciated.







share|cite|improve this question





















  • I am not familiar with random variables. Are you actually stuck at the point of differentiation?
    – Szeto
    Aug 1 at 2:05










  • Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
    – Kashan
    Aug 1 at 3:04












up vote
0
down vote

favorite
1









up vote
0
down vote

favorite
1






1





Following my question here, I am able to solve up to a point beyond which I would really appreciate any help (also if my current understanding is right).



Note that I have to find $f_T(t)$. The question starts with:



$$P(T<t) = 1-int_mathcalVexp(-lambdapi v^2t^2)dP_V(v).$$



with $T, V$ are random variables with values $t,v$ denoting time and speed. $mathcalV$ is the range of $V$. $lambda$ is a rate (constant).
The final answer should be:



$$f_T(t) = fracg(v_min) - g(v_max)(v_max - v_min)t, tgeq0$$
where $$g(x) = xe^-lambda pi t^2x^2 + frac1sqrtlambdatQ(sqrt2pilambda t x)$$ and $$Q(x) = frac1sqrt2piint_x^infty e^fracu^22du$$




My Solution



Let velocity be a continous uniform distribution with range $[v_min,v_max] = [v_0,v_1]$, so above eq. would become:



$$P(T<t) = 1-int_v_0^v_1exp(-lambdapi v^2t^2)Big(frac1v_1-v_0Big)dv.$$



$$f_T(t) = -Big(frac1v_1-v_0Big)fracddtint_v_0^v_1exp(-lambdapi v^2t^2) dv.$$



using the property $int e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[texterf(sqrtpilambda tv_1) - texterf(sqrtpilambda tv_0)].$$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[Q(sqrtpilambda tv_0) - Q(sqrtpilambda tv_1)].$$



I cannot reach beyond this point. Any help would be much appreciated.







share|cite|improve this question













Following my question here, I am able to solve up to a point beyond which I would really appreciate any help (also if my current understanding is right).



Note that I have to find $f_T(t)$. The question starts with:



$$P(T<t) = 1-int_mathcalVexp(-lambdapi v^2t^2)dP_V(v).$$



with $T, V$ are random variables with values $t,v$ denoting time and speed. $mathcalV$ is the range of $V$. $lambda$ is a rate (constant).
The final answer should be:



$$f_T(t) = fracg(v_min) - g(v_max)(v_max - v_min)t, tgeq0$$
where $$g(x) = xe^-lambda pi t^2x^2 + frac1sqrtlambdatQ(sqrt2pilambda t x)$$ and $$Q(x) = frac1sqrt2piint_x^infty e^fracu^22du$$




My Solution



Let velocity be a continous uniform distribution with range $[v_min,v_max] = [v_0,v_1]$, so above eq. would become:



$$P(T<t) = 1-int_v_0^v_1exp(-lambdapi v^2t^2)Big(frac1v_1-v_0Big)dv.$$



$$f_T(t) = -Big(frac1v_1-v_0Big)fracddtint_v_0^v_1exp(-lambdapi v^2t^2) dv.$$



using the property $int e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[texterf(sqrtpilambda tv_1) - texterf(sqrtpilambda tv_0)].$$



$$f_T(t) = -Big(frac1(v_1-v_0)2sqrtlambdaBig)fracddtfrac1t[Q(sqrtpilambda tv_0) - Q(sqrtpilambda tv_1)].$$



I cannot reach beyond this point. Any help would be much appreciated.









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share|cite|improve this question




share|cite|improve this question








edited Aug 1 at 5:20
























asked Jul 31 at 23:31









Kashan

341110




341110











  • I am not familiar with random variables. Are you actually stuck at the point of differentiation?
    – Szeto
    Aug 1 at 2:05










  • Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
    – Kashan
    Aug 1 at 3:04
















  • I am not familiar with random variables. Are you actually stuck at the point of differentiation?
    – Szeto
    Aug 1 at 2:05










  • Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
    – Kashan
    Aug 1 at 3:04















I am not familiar with random variables. Are you actually stuck at the point of differentiation?
– Szeto
Aug 1 at 2:05




I am not familiar with random variables. Are you actually stuck at the point of differentiation?
– Szeto
Aug 1 at 2:05












Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
– Kashan
Aug 1 at 3:04




Yes. I need the final solution by solving integral and derivate. for random variable, please consider $t,v$ as some variables
– Kashan
Aug 1 at 3:04










1 Answer
1






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oldest

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up vote
2
down vote



accepted











Using the property $e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$




This is wrong. Look up the definition of error function.




Basically, you just need to find $fracddtP(t)$.



Let $$I(t) = int_v_0^v_1exp(-lambdapi v^2t^2)dv$$
(So, $P(t)=1-frac1v_1-v_0I(t)$)




Using the substitution $u=vt$,
$$I(t)=frac1tint_v_0t^v_1texp(-lambdapi u^2)du$$



By Fundamental Theorem of Calculus, this also equals
$$I(t)=frac1tleft(intexp(-lambdapi (v_1t)^2),,v_1dt-intexp(-lambdapi (v_0t)^2),,v_0dtright)$$



Applying chain rule,
$$I'(t)=fracI(t)+tv_1exp(-lambdapi (v_1t)^2)-tv_0exp(-lambdapi (v_0t)^2)t^2$$




The problem is basically solved, now it is a problem to fit in your notations.



Note that $$I(t)=sqrt2piQ(sqrt2lambdapiv_0t)-sqrt2piQ(sqrt2lambdapiv_1t)$$



...your notations are very messy...try to fit in yourself.






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    1 Answer
    1






    active

    oldest

    votes








    1 Answer
    1






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes








    up vote
    2
    down vote



    accepted











    Using the property $e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$




    This is wrong. Look up the definition of error function.




    Basically, you just need to find $fracddtP(t)$.



    Let $$I(t) = int_v_0^v_1exp(-lambdapi v^2t^2)dv$$
    (So, $P(t)=1-frac1v_1-v_0I(t)$)




    Using the substitution $u=vt$,
    $$I(t)=frac1tint_v_0t^v_1texp(-lambdapi u^2)du$$



    By Fundamental Theorem of Calculus, this also equals
    $$I(t)=frac1tleft(intexp(-lambdapi (v_1t)^2),,v_1dt-intexp(-lambdapi (v_0t)^2),,v_0dtright)$$



    Applying chain rule,
    $$I'(t)=fracI(t)+tv_1exp(-lambdapi (v_1t)^2)-tv_0exp(-lambdapi (v_0t)^2)t^2$$




    The problem is basically solved, now it is a problem to fit in your notations.



    Note that $$I(t)=sqrt2piQ(sqrt2lambdapiv_0t)-sqrt2piQ(sqrt2lambdapiv_1t)$$



    ...your notations are very messy...try to fit in yourself.






    share|cite|improve this answer

























      up vote
      2
      down vote



      accepted











      Using the property $e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$




      This is wrong. Look up the definition of error function.




      Basically, you just need to find $fracddtP(t)$.



      Let $$I(t) = int_v_0^v_1exp(-lambdapi v^2t^2)dv$$
      (So, $P(t)=1-frac1v_1-v_0I(t)$)




      Using the substitution $u=vt$,
      $$I(t)=frac1tint_v_0t^v_1texp(-lambdapi u^2)du$$



      By Fundamental Theorem of Calculus, this also equals
      $$I(t)=frac1tleft(intexp(-lambdapi (v_1t)^2),,v_1dt-intexp(-lambdapi (v_0t)^2),,v_0dtright)$$



      Applying chain rule,
      $$I'(t)=fracI(t)+tv_1exp(-lambdapi (v_1t)^2)-tv_0exp(-lambdapi (v_0t)^2)t^2$$




      The problem is basically solved, now it is a problem to fit in your notations.



      Note that $$I(t)=sqrt2piQ(sqrt2lambdapiv_0t)-sqrt2piQ(sqrt2lambdapiv_1t)$$



      ...your notations are very messy...try to fit in yourself.






      share|cite|improve this answer























        up vote
        2
        down vote



        accepted







        up vote
        2
        down vote



        accepted







        Using the property $e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$




        This is wrong. Look up the definition of error function.




        Basically, you just need to find $fracddtP(t)$.



        Let $$I(t) = int_v_0^v_1exp(-lambdapi v^2t^2)dv$$
        (So, $P(t)=1-frac1v_1-v_0I(t)$)




        Using the substitution $u=vt$,
        $$I(t)=frac1tint_v_0t^v_1texp(-lambdapi u^2)du$$



        By Fundamental Theorem of Calculus, this also equals
        $$I(t)=frac1tleft(intexp(-lambdapi (v_1t)^2),,v_1dt-intexp(-lambdapi (v_0t)^2),,v_0dtright)$$



        Applying chain rule,
        $$I'(t)=fracI(t)+tv_1exp(-lambdapi (v_1t)^2)-tv_0exp(-lambdapi (v_0t)^2)t^2$$




        The problem is basically solved, now it is a problem to fit in your notations.



        Note that $$I(t)=sqrt2piQ(sqrt2lambdapiv_0t)-sqrt2piQ(sqrt2lambdapiv_1t)$$



        ...your notations are very messy...try to fit in yourself.






        share|cite|improve this answer














        Using the property $e^-cx^2 = sqrtfracpi4c erf(sqrtcx)$




        This is wrong. Look up the definition of error function.




        Basically, you just need to find $fracddtP(t)$.



        Let $$I(t) = int_v_0^v_1exp(-lambdapi v^2t^2)dv$$
        (So, $P(t)=1-frac1v_1-v_0I(t)$)




        Using the substitution $u=vt$,
        $$I(t)=frac1tint_v_0t^v_1texp(-lambdapi u^2)du$$



        By Fundamental Theorem of Calculus, this also equals
        $$I(t)=frac1tleft(intexp(-lambdapi (v_1t)^2),,v_1dt-intexp(-lambdapi (v_0t)^2),,v_0dtright)$$



        Applying chain rule,
        $$I'(t)=fracI(t)+tv_1exp(-lambdapi (v_1t)^2)-tv_0exp(-lambdapi (v_0t)^2)t^2$$




        The problem is basically solved, now it is a problem to fit in your notations.



        Note that $$I(t)=sqrt2piQ(sqrt2lambdapiv_0t)-sqrt2piQ(sqrt2lambdapiv_1t)$$



        ...your notations are very messy...try to fit in yourself.







        share|cite|improve this answer













        share|cite|improve this answer



        share|cite|improve this answer











        answered Aug 1 at 3:35









        Szeto

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