How to prove $E[g(x)] = int_0^infty g'(x)S(x) dx$ Announcing the arrival of Valued Associate #679: Cesar Manara Planned maintenance scheduled April 23, 2019 at 23:30 UTC (7:30pm US/Eastern)Is it true that $limlimits_xtoinftyx·P[X>x]=0$?Proof of $textTVaR_p(X)$ and $textVaR_u(X)$ relationshipShow that if X is a continuous random variable on $[b,infty)$ then $mathrmE[X]=b+int_b^infty(1- F(x))dx $For a pdf $f(x)$, how can we prove that $int_-infty^infty x,f(x),dx=int_-infty^infty F(xgeq t),dt$?Prove the following equality to show a relationship between Poisson and Gamma Random VariablesHow can I prove that expectation of conditional random variable?Peculiar problem about characteristic function and density function.With scant information, how to prove this probability limit tends to zero?How to prove that a conditional pdf sums to 1?How to calculate a joint pdf by convolutionFind the conditional density function and expectation of $Y$ given $X$ when $f(x,y) = lambda^2e^-lambda y$ and $f(x,y) = xe^-x(y+1)$

C's equality operator on converted pointers

Does "shooting for effect" have contradictory meanings in different areas?

Did any compiler fully use 80-bit floating point?

Why are my pictures showing a dark band on one edge?

Draw 4 of the same figure in the same tikzpicture

What is the meaning of 'breadth' in breadth first search?

Is it fair for a professor to grade us on the possession of past papers?

Central Vacuuming: Is it worth it, and how does it compare to normal vacuuming?

Intuitive explanation of the rank-nullity theorem

What does Turing mean by this statement?

Why weren't discrete x86 CPUs ever used in game hardware?

Misunderstanding of Sylow theory

Is there public access to the Meteor Crater in Arizona?

What are the discoveries that have been possible with the rejection of positivism?

A letter with no particular backstory

Dyck paths with extra diagonals from valleys (Laser construction)

Would it be easier to apply for a UK visa if there is a host family to sponsor for you in going there?

Karn the great creator - 'card from outside the game' in sealed

Do wooden building fires get hotter than 600°C?

How many morphisms from 1 to 1+1 can there be?

Co-worker has annoying ringtone

Drawing spherical mirrors

What makes a man succeed?

How to identify unknown coordinate type and convert to lat/lon?



How to prove $E[g(x)] = int_0^infty g'(x)S(x) dx$



Announcing the arrival of Valued Associate #679: Cesar Manara
Planned maintenance scheduled April 23, 2019 at 23:30 UTC (7:30pm US/Eastern)Is it true that $limlimits_xtoinftyx·P[X>x]=0$?Proof of $textTVaR_p(X)$ and $textVaR_u(X)$ relationshipShow that if X is a continuous random variable on $[b,infty)$ then $mathrmE[X]=b+int_b^infty(1- F(x))dx $For a pdf $f(x)$, how can we prove that $int_-infty^infty x,f(x),dx=int_-infty^infty F(xgeq t),dt$?Prove the following equality to show a relationship between Poisson and Gamma Random VariablesHow can I prove that expectation of conditional random variable?Peculiar problem about characteristic function and density function.With scant information, how to prove this probability limit tends to zero?How to prove that a conditional pdf sums to 1?How to calculate a joint pdf by convolutionFind the conditional density function and expectation of $Y$ given $X$ when $f(x,y) = lambda^2e^-lambda y$ and $f(x,y) = xe^-x(y+1)$










1












$begingroup$


Given that $E[g(X)] = int_-infty^infty g(x)f(x) dx$, how to prove $E[g(X)] = int_0^infty g'(x)S(x)dx$, where $S(x) = 1-F(x)$?



By integration by parts, I can get the following:
beginalign
E[g(X)] &= int_-infty^infty g(x)f(x) dx \
&= int_-infty^infty g(x)F'(x) dx \
&= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)F(x) dx \
&= g(x)F(x)|_-infty^infty + int_-infty^infty g'(x)[1-S(x)] dx \
&= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)dx +int_-infty^infty g'(x)S(x) dx\
endalign



Then I am stuck.










share|cite|improve this question









$endgroup$
















    1












    $begingroup$


    Given that $E[g(X)] = int_-infty^infty g(x)f(x) dx$, how to prove $E[g(X)] = int_0^infty g'(x)S(x)dx$, where $S(x) = 1-F(x)$?



    By integration by parts, I can get the following:
    beginalign
    E[g(X)] &= int_-infty^infty g(x)f(x) dx \
    &= int_-infty^infty g(x)F'(x) dx \
    &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)F(x) dx \
    &= g(x)F(x)|_-infty^infty + int_-infty^infty g'(x)[1-S(x)] dx \
    &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)dx +int_-infty^infty g'(x)S(x) dx\
    endalign



    Then I am stuck.










    share|cite|improve this question









    $endgroup$














      1












      1








      1


      2



      $begingroup$


      Given that $E[g(X)] = int_-infty^infty g(x)f(x) dx$, how to prove $E[g(X)] = int_0^infty g'(x)S(x)dx$, where $S(x) = 1-F(x)$?



      By integration by parts, I can get the following:
      beginalign
      E[g(X)] &= int_-infty^infty g(x)f(x) dx \
      &= int_-infty^infty g(x)F'(x) dx \
      &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)F(x) dx \
      &= g(x)F(x)|_-infty^infty + int_-infty^infty g'(x)[1-S(x)] dx \
      &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)dx +int_-infty^infty g'(x)S(x) dx\
      endalign



      Then I am stuck.










      share|cite|improve this question









      $endgroup$




      Given that $E[g(X)] = int_-infty^infty g(x)f(x) dx$, how to prove $E[g(X)] = int_0^infty g'(x)S(x)dx$, where $S(x) = 1-F(x)$?



      By integration by parts, I can get the following:
      beginalign
      E[g(X)] &= int_-infty^infty g(x)f(x) dx \
      &= int_-infty^infty g(x)F'(x) dx \
      &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)F(x) dx \
      &= g(x)F(x)|_-infty^infty + int_-infty^infty g'(x)[1-S(x)] dx \
      &= g(x)F(x)|_-infty^infty - int_-infty^infty g'(x)dx +int_-infty^infty g'(x)S(x) dx\
      endalign



      Then I am stuck.







      probability






      share|cite|improve this question













      share|cite|improve this question











      share|cite|improve this question




      share|cite|improve this question










      asked Apr 2 at 0:18









      JangoJango

      1839




      1839




















          2 Answers
          2






          active

          oldest

          votes


















          3












          $begingroup$

          I think what you are trying to prove is not exactly correct. I will work through the problem and show the correct answer at the end.



          You need to split the integral into two, one for the region $xge 0$ and one for $xle 0$.



          In the positive region, instead of writing $f(x)=F'(x)$ and integrating by parts, you need to use $f=(F(x)-1)'$. This is the only choice which ensures that the resulting integral actually exists; note that $F(x)-1$ goes to zero as $xto+infty$, but $F(x)$ does not.



          beginalign
          int_0^infty g(x)f(x),dx
          &=int_0^infty g(x)[F(x)-1]',dx
          \&=g(x)[F(x)-1]Big|^infty_0-int_0^infty g'(s)[F(x)-1],dx
          \&=underbraceBig(lim_xtoinftyg(x)[F(x)-1]Big)_=0-g(0)[F(0)-1]+int_0^infty g'(x)S(x),dx
          endalign

          It takes some doing, but you can show that that limit actually is zero, as long as $E[g(X)]$ is finite. See Is it true that $limlimits_xtoinftyx·P[X>x]=0$? for some inspiration. Edit: Actually, I am not quite sure this is true without some additional assumptions on $g.$ It is true as long as $g$ is either bounded or monotonic.



          For the negative region, you do want to use $F(x)$ as the antiderivate of $f(x)$, because $lim_xto-inftyF(x)=0$.
          beginalign
          int_-infty^0 g(x)f(x),dx
          &=int_-infty^0 g(x)F(x)',dx
          \&=g(x)F(x)Big|^0_-infty-int_-infty^0 g'(s)F(x),dx
          \&=g(0)F(0)-underbraceBig(lim_xto-inftyg(x)F(x)Big)_=0-int_-infty^0 g'(x)F(x),dx
          endalign

          Putting this all together, we get
          $$
          bbox[7px,border:2px solid red]int_-infty^infty g(x)f(x),dx=g(0)+int_0^infty g'(x)S(x),dx-int_-infty^0g'(x)F(x),dx
          $$

          This is correct for any function $g$ such that $E[g(X)]$ is finite. Edit: Well, as long as $g$ is either bounded or monotonic.



          If we make further assumptions about $g$, we can write this more nicely. Assuming $g(-infty):=lim_xto-inftyg(x)$ exists, you would have
          $$
          g(0)=g(-infty)+int_-infty^0 g'(x),dx
          $$

          so
          $$
          bbox[7px,border:2px solid green]int_-infty^infty g(x)f(x),dx=g(-infty)+int_-infty^infty g'(x)S(x),dx
          $$

          You cannot in general avoid the presence of some constant $g(a)$. This is because the $int g'(x)S(x),dx$ part of the formula does not change when $g$ is shifted by a constant (this does not affect $g'$), but $E[g(x)]$ does change when $g$ is shifted by a constant.






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
            $endgroup$
            – Jango
            Apr 2 at 14:34










          • $begingroup$
            @Jango Can I ask where this appears in the book?
            $endgroup$
            – Mike Earnest
            Apr 2 at 14:48


















          1












          $begingroup$

          Write $1-F(x)=int_(x,infty) dmu(y)$ where $mu$ is the measure corresponding to $F$. Now apply Fubini/Tonelli Theorem to the right hand side.






          share|cite|improve this answer









          $endgroup$













            Your Answer








            StackExchange.ready(function()
            var channelOptions =
            tags: "".split(" "),
            id: "69"
            ;
            initTagRenderer("".split(" "), "".split(" "), channelOptions);

            StackExchange.using("externalEditor", function()
            // Have to fire editor after snippets, if snippets enabled
            if (StackExchange.settings.snippets.snippetsEnabled)
            StackExchange.using("snippets", function()
            createEditor();
            );

            else
            createEditor();

            );

            function createEditor()
            StackExchange.prepareEditor(
            heartbeatType: 'answer',
            autoActivateHeartbeat: false,
            convertImagesToLinks: true,
            noModals: true,
            showLowRepImageUploadWarning: true,
            reputationToPostImages: 10,
            bindNavPrevention: true,
            postfix: "",
            imageUploader:
            brandingHtml: "Powered by u003ca class="icon-imgur-white" href="https://imgur.com/"u003eu003c/au003e",
            contentPolicyHtml: "User contributions licensed under u003ca href="https://creativecommons.org/licenses/by-sa/3.0/"u003ecc by-sa 3.0 with attribution requiredu003c/au003e u003ca href="https://stackoverflow.com/legal/content-policy"u003e(content policy)u003c/au003e",
            allowUrls: true
            ,
            noCode: true, onDemand: true,
            discardSelector: ".discard-answer"
            ,immediatelyShowMarkdownHelp:true
            );



            );













            draft saved

            draft discarded


















            StackExchange.ready(
            function ()
            StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3171308%2fhow-to-prove-egx-int-0-infty-gxsx-dx%23new-answer', 'question_page');

            );

            Post as a guest















            Required, but never shown

























            2 Answers
            2






            active

            oldest

            votes








            2 Answers
            2






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes









            3












            $begingroup$

            I think what you are trying to prove is not exactly correct. I will work through the problem and show the correct answer at the end.



            You need to split the integral into two, one for the region $xge 0$ and one for $xle 0$.



            In the positive region, instead of writing $f(x)=F'(x)$ and integrating by parts, you need to use $f=(F(x)-1)'$. This is the only choice which ensures that the resulting integral actually exists; note that $F(x)-1$ goes to zero as $xto+infty$, but $F(x)$ does not.



            beginalign
            int_0^infty g(x)f(x),dx
            &=int_0^infty g(x)[F(x)-1]',dx
            \&=g(x)[F(x)-1]Big|^infty_0-int_0^infty g'(s)[F(x)-1],dx
            \&=underbraceBig(lim_xtoinftyg(x)[F(x)-1]Big)_=0-g(0)[F(0)-1]+int_0^infty g'(x)S(x),dx
            endalign

            It takes some doing, but you can show that that limit actually is zero, as long as $E[g(X)]$ is finite. See Is it true that $limlimits_xtoinftyx·P[X>x]=0$? for some inspiration. Edit: Actually, I am not quite sure this is true without some additional assumptions on $g.$ It is true as long as $g$ is either bounded or monotonic.



            For the negative region, you do want to use $F(x)$ as the antiderivate of $f(x)$, because $lim_xto-inftyF(x)=0$.
            beginalign
            int_-infty^0 g(x)f(x),dx
            &=int_-infty^0 g(x)F(x)',dx
            \&=g(x)F(x)Big|^0_-infty-int_-infty^0 g'(s)F(x),dx
            \&=g(0)F(0)-underbraceBig(lim_xto-inftyg(x)F(x)Big)_=0-int_-infty^0 g'(x)F(x),dx
            endalign

            Putting this all together, we get
            $$
            bbox[7px,border:2px solid red]int_-infty^infty g(x)f(x),dx=g(0)+int_0^infty g'(x)S(x),dx-int_-infty^0g'(x)F(x),dx
            $$

            This is correct for any function $g$ such that $E[g(X)]$ is finite. Edit: Well, as long as $g$ is either bounded or monotonic.



            If we make further assumptions about $g$, we can write this more nicely. Assuming $g(-infty):=lim_xto-inftyg(x)$ exists, you would have
            $$
            g(0)=g(-infty)+int_-infty^0 g'(x),dx
            $$

            so
            $$
            bbox[7px,border:2px solid green]int_-infty^infty g(x)f(x),dx=g(-infty)+int_-infty^infty g'(x)S(x),dx
            $$

            You cannot in general avoid the presence of some constant $g(a)$. This is because the $int g'(x)S(x),dx$ part of the formula does not change when $g$ is shifted by a constant (this does not affect $g'$), but $E[g(x)]$ does change when $g$ is shifted by a constant.






            share|cite|improve this answer











            $endgroup$












            • $begingroup$
              Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
              $endgroup$
              – Jango
              Apr 2 at 14:34










            • $begingroup$
              @Jango Can I ask where this appears in the book?
              $endgroup$
              – Mike Earnest
              Apr 2 at 14:48















            3












            $begingroup$

            I think what you are trying to prove is not exactly correct. I will work through the problem and show the correct answer at the end.



            You need to split the integral into two, one for the region $xge 0$ and one for $xle 0$.



            In the positive region, instead of writing $f(x)=F'(x)$ and integrating by parts, you need to use $f=(F(x)-1)'$. This is the only choice which ensures that the resulting integral actually exists; note that $F(x)-1$ goes to zero as $xto+infty$, but $F(x)$ does not.



            beginalign
            int_0^infty g(x)f(x),dx
            &=int_0^infty g(x)[F(x)-1]',dx
            \&=g(x)[F(x)-1]Big|^infty_0-int_0^infty g'(s)[F(x)-1],dx
            \&=underbraceBig(lim_xtoinftyg(x)[F(x)-1]Big)_=0-g(0)[F(0)-1]+int_0^infty g'(x)S(x),dx
            endalign

            It takes some doing, but you can show that that limit actually is zero, as long as $E[g(X)]$ is finite. See Is it true that $limlimits_xtoinftyx·P[X>x]=0$? for some inspiration. Edit: Actually, I am not quite sure this is true without some additional assumptions on $g.$ It is true as long as $g$ is either bounded or monotonic.



            For the negative region, you do want to use $F(x)$ as the antiderivate of $f(x)$, because $lim_xto-inftyF(x)=0$.
            beginalign
            int_-infty^0 g(x)f(x),dx
            &=int_-infty^0 g(x)F(x)',dx
            \&=g(x)F(x)Big|^0_-infty-int_-infty^0 g'(s)F(x),dx
            \&=g(0)F(0)-underbraceBig(lim_xto-inftyg(x)F(x)Big)_=0-int_-infty^0 g'(x)F(x),dx
            endalign

            Putting this all together, we get
            $$
            bbox[7px,border:2px solid red]int_-infty^infty g(x)f(x),dx=g(0)+int_0^infty g'(x)S(x),dx-int_-infty^0g'(x)F(x),dx
            $$

            This is correct for any function $g$ such that $E[g(X)]$ is finite. Edit: Well, as long as $g$ is either bounded or monotonic.



            If we make further assumptions about $g$, we can write this more nicely. Assuming $g(-infty):=lim_xto-inftyg(x)$ exists, you would have
            $$
            g(0)=g(-infty)+int_-infty^0 g'(x),dx
            $$

            so
            $$
            bbox[7px,border:2px solid green]int_-infty^infty g(x)f(x),dx=g(-infty)+int_-infty^infty g'(x)S(x),dx
            $$

            You cannot in general avoid the presence of some constant $g(a)$. This is because the $int g'(x)S(x),dx$ part of the formula does not change when $g$ is shifted by a constant (this does not affect $g'$), but $E[g(x)]$ does change when $g$ is shifted by a constant.






            share|cite|improve this answer











            $endgroup$












            • $begingroup$
              Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
              $endgroup$
              – Jango
              Apr 2 at 14:34










            • $begingroup$
              @Jango Can I ask where this appears in the book?
              $endgroup$
              – Mike Earnest
              Apr 2 at 14:48













            3












            3








            3





            $begingroup$

            I think what you are trying to prove is not exactly correct. I will work through the problem and show the correct answer at the end.



            You need to split the integral into two, one for the region $xge 0$ and one for $xle 0$.



            In the positive region, instead of writing $f(x)=F'(x)$ and integrating by parts, you need to use $f=(F(x)-1)'$. This is the only choice which ensures that the resulting integral actually exists; note that $F(x)-1$ goes to zero as $xto+infty$, but $F(x)$ does not.



            beginalign
            int_0^infty g(x)f(x),dx
            &=int_0^infty g(x)[F(x)-1]',dx
            \&=g(x)[F(x)-1]Big|^infty_0-int_0^infty g'(s)[F(x)-1],dx
            \&=underbraceBig(lim_xtoinftyg(x)[F(x)-1]Big)_=0-g(0)[F(0)-1]+int_0^infty g'(x)S(x),dx
            endalign

            It takes some doing, but you can show that that limit actually is zero, as long as $E[g(X)]$ is finite. See Is it true that $limlimits_xtoinftyx·P[X>x]=0$? for some inspiration. Edit: Actually, I am not quite sure this is true without some additional assumptions on $g.$ It is true as long as $g$ is either bounded or monotonic.



            For the negative region, you do want to use $F(x)$ as the antiderivate of $f(x)$, because $lim_xto-inftyF(x)=0$.
            beginalign
            int_-infty^0 g(x)f(x),dx
            &=int_-infty^0 g(x)F(x)',dx
            \&=g(x)F(x)Big|^0_-infty-int_-infty^0 g'(s)F(x),dx
            \&=g(0)F(0)-underbraceBig(lim_xto-inftyg(x)F(x)Big)_=0-int_-infty^0 g'(x)F(x),dx
            endalign

            Putting this all together, we get
            $$
            bbox[7px,border:2px solid red]int_-infty^infty g(x)f(x),dx=g(0)+int_0^infty g'(x)S(x),dx-int_-infty^0g'(x)F(x),dx
            $$

            This is correct for any function $g$ such that $E[g(X)]$ is finite. Edit: Well, as long as $g$ is either bounded or monotonic.



            If we make further assumptions about $g$, we can write this more nicely. Assuming $g(-infty):=lim_xto-inftyg(x)$ exists, you would have
            $$
            g(0)=g(-infty)+int_-infty^0 g'(x),dx
            $$

            so
            $$
            bbox[7px,border:2px solid green]int_-infty^infty g(x)f(x),dx=g(-infty)+int_-infty^infty g'(x)S(x),dx
            $$

            You cannot in general avoid the presence of some constant $g(a)$. This is because the $int g'(x)S(x),dx$ part of the formula does not change when $g$ is shifted by a constant (this does not affect $g'$), but $E[g(x)]$ does change when $g$ is shifted by a constant.






            share|cite|improve this answer











            $endgroup$



            I think what you are trying to prove is not exactly correct. I will work through the problem and show the correct answer at the end.



            You need to split the integral into two, one for the region $xge 0$ and one for $xle 0$.



            In the positive region, instead of writing $f(x)=F'(x)$ and integrating by parts, you need to use $f=(F(x)-1)'$. This is the only choice which ensures that the resulting integral actually exists; note that $F(x)-1$ goes to zero as $xto+infty$, but $F(x)$ does not.



            beginalign
            int_0^infty g(x)f(x),dx
            &=int_0^infty g(x)[F(x)-1]',dx
            \&=g(x)[F(x)-1]Big|^infty_0-int_0^infty g'(s)[F(x)-1],dx
            \&=underbraceBig(lim_xtoinftyg(x)[F(x)-1]Big)_=0-g(0)[F(0)-1]+int_0^infty g'(x)S(x),dx
            endalign

            It takes some doing, but you can show that that limit actually is zero, as long as $E[g(X)]$ is finite. See Is it true that $limlimits_xtoinftyx·P[X>x]=0$? for some inspiration. Edit: Actually, I am not quite sure this is true without some additional assumptions on $g.$ It is true as long as $g$ is either bounded or monotonic.



            For the negative region, you do want to use $F(x)$ as the antiderivate of $f(x)$, because $lim_xto-inftyF(x)=0$.
            beginalign
            int_-infty^0 g(x)f(x),dx
            &=int_-infty^0 g(x)F(x)',dx
            \&=g(x)F(x)Big|^0_-infty-int_-infty^0 g'(s)F(x),dx
            \&=g(0)F(0)-underbraceBig(lim_xto-inftyg(x)F(x)Big)_=0-int_-infty^0 g'(x)F(x),dx
            endalign

            Putting this all together, we get
            $$
            bbox[7px,border:2px solid red]int_-infty^infty g(x)f(x),dx=g(0)+int_0^infty g'(x)S(x),dx-int_-infty^0g'(x)F(x),dx
            $$

            This is correct for any function $g$ such that $E[g(X)]$ is finite. Edit: Well, as long as $g$ is either bounded or monotonic.



            If we make further assumptions about $g$, we can write this more nicely. Assuming $g(-infty):=lim_xto-inftyg(x)$ exists, you would have
            $$
            g(0)=g(-infty)+int_-infty^0 g'(x),dx
            $$

            so
            $$
            bbox[7px,border:2px solid green]int_-infty^infty g(x)f(x),dx=g(-infty)+int_-infty^infty g'(x)S(x),dx
            $$

            You cannot in general avoid the presence of some constant $g(a)$. This is because the $int g'(x)S(x),dx$ part of the formula does not change when $g$ is shifted by a constant (this does not affect $g'$), but $E[g(x)]$ does change when $g$ is shifted by a constant.







            share|cite|improve this answer














            share|cite|improve this answer



            share|cite|improve this answer








            edited Apr 2 at 4:54

























            answered Apr 2 at 4:27









            Mike EarnestMike Earnest

            28.2k22152




            28.2k22152











            • $begingroup$
              Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
              $endgroup$
              – Jango
              Apr 2 at 14:34










            • $begingroup$
              @Jango Can I ask where this appears in the book?
              $endgroup$
              – Mike Earnest
              Apr 2 at 14:48
















            • $begingroup$
              Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
              $endgroup$
              – Jango
              Apr 2 at 14:34










            • $begingroup$
              @Jango Can I ask where this appears in the book?
              $endgroup$
              – Mike Earnest
              Apr 2 at 14:48















            $begingroup$
            Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
            $endgroup$
            – Jango
            Apr 2 at 14:34




            $begingroup$
            Thank you very much. I did not think it is so difficult since I read this from "Loss Model" other than analysis. Anyway, your work is clear and easy to understand. Thanks.
            $endgroup$
            – Jango
            Apr 2 at 14:34












            $begingroup$
            @Jango Can I ask where this appears in the book?
            $endgroup$
            – Mike Earnest
            Apr 2 at 14:48




            $begingroup$
            @Jango Can I ask where this appears in the book?
            $endgroup$
            – Mike Earnest
            Apr 2 at 14:48











            1












            $begingroup$

            Write $1-F(x)=int_(x,infty) dmu(y)$ where $mu$ is the measure corresponding to $F$. Now apply Fubini/Tonelli Theorem to the right hand side.






            share|cite|improve this answer









            $endgroup$

















              1












              $begingroup$

              Write $1-F(x)=int_(x,infty) dmu(y)$ where $mu$ is the measure corresponding to $F$. Now apply Fubini/Tonelli Theorem to the right hand side.






              share|cite|improve this answer









              $endgroup$















                1












                1








                1





                $begingroup$

                Write $1-F(x)=int_(x,infty) dmu(y)$ where $mu$ is the measure corresponding to $F$. Now apply Fubini/Tonelli Theorem to the right hand side.






                share|cite|improve this answer









                $endgroup$



                Write $1-F(x)=int_(x,infty) dmu(y)$ where $mu$ is the measure corresponding to $F$. Now apply Fubini/Tonelli Theorem to the right hand side.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Apr 2 at 0:22









                Kavi Rama MurthyKavi Rama Murthy

                76.1k53370




                76.1k53370



























                    draft saved

                    draft discarded
















































                    Thanks for contributing an answer to Mathematics Stack Exchange!


                    • Please be sure to answer the question. Provide details and share your research!

                    But avoid


                    • Asking for help, clarification, or responding to other answers.

                    • Making statements based on opinion; back them up with references or personal experience.

                    Use MathJax to format equations. MathJax reference.


                    To learn more, see our tips on writing great answers.




                    draft saved


                    draft discarded














                    StackExchange.ready(
                    function ()
                    StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3171308%2fhow-to-prove-egx-int-0-infty-gxsx-dx%23new-answer', 'question_page');

                    );

                    Post as a guest















                    Required, but never shown





















































                    Required, but never shown














                    Required, but never shown












                    Required, but never shown







                    Required, but never shown

































                    Required, but never shown














                    Required, but never shown












                    Required, but never shown







                    Required, but never shown







                    Popular posts from this blog

                    Triangular numbers and gcdProving sum of a set is $0 pmod n$ if $n$ is odd, or $fracn2 pmod n$ if $n$ is even?Is greatest common divisor of two numbers really their smallest linear combination?GCD, LCM RelationshipProve a set of nonnegative integers with greatest common divisor 1 and closed under addition has all but finite many nonnegative integers.all pairs of a and b in an equation containing gcdTriangular Numbers Modulo $k$ - Hit All Values?Understanding the Existence and Uniqueness of the GCDGCD and LCM with logical symbolsThe greatest common divisor of two positive integers less than 100 is equal to 3. Their least common multiple is twelve times one of the integers.Suppose that for all integers $x$, $x|a$ and $x|b$ if and only if $x|c$. Then $c = gcd(a,b)$Which is the gcd of 2 numbers which are multiplied and the result is 600000?

                    Barbados Ynhâld Skiednis | Geografy | Demografy | Navigaasjemenu

                    Србија Садржај Етимологија Географија Историја Политички систем и уставно-правно уређење Становништво Привреда Образовање Култура Спорт Државни празници Галерија Напомене Референце Литература Спољашње везе Мени за навигацију44°48′N 20°28′E / 44.800° СГШ; 20.467° ИГД / 44.800; 20.46744°48′N 20°28′E / 44.800° СГШ; 20.467° ИГД / 44.800; 20.467ууРезултати пописа 2011. према старости и полуу„Положај, рељеф и клима”„Europe: Serbia”„Основни подаци”„Gross domestic product based on purchasing-power-parity (PPP) valuation of country GDP”„Human Development Report 2018 – "Human Development Indices and Indicators 6”„Устав Републике Србије”Правопис српскога језикаGoogle DriveComparative Hungarian Cultural StudiesCalcium and Magnesium in Groundwater: Occurrence and Significance for Human Health„UNSD — Methodology”„Процене становништва | Републички завод за статистику Србије”The Age of Nepotism: Travel Journals and Observations from the Balkans During the Depression„The Serbian Revolution and the Serbian State”„Устав Србије”„Serbia a few steps away from concluding WTO accession negotiations”„A credible enlargement perspective for and enhanced EU engagement with the Western Balkans”„Freedom in the World 2017”„Serbia: On the Way to EU Accession”„Human Development Indices and Indicators: 2018 Statistical Update”„2018 Social Progress Index”„Global Peace Index”Sabres of Two Easts: An Untold History of Muslims in Eastern Europe, Their Friends and Foes„Пројекат Растко—Лузица”„Serbia: Introduction”„Serbia”оригинала„The World Factbook: Serbia”„The World Factbook: Kosovo”„Border Police Department”„Uredba o kontroli prelaska administrativne linije prema Autonomnoj pokrajini Kosovo i Metohija”оригиналаIvana Carevic, Velimir Jovanovic, STRATIGRAPHIC-STRUCTURAL CHARACTERISTICS OF MAČVA BASIN, UDC 911.2:551.7(497.11), pp. 1Archived„About the Carpathians – Carpathian Heritage Society”оригинала„O Srbiji”оригинала„Статистички годишњак Србије, 2009: Географски прегледГеографија за осми разред основне школе„Отворена, електронска база едукационих радова”„Влада Републике Србије: Положај, рељеф и клима”„Копрен (Стара планина)”„Туристичка дестинација-Србија”„Висина водопада”„РХМЗ — Републички Хидрометеоролошки завод Србије Кнеза Вишеслава 66 Београд”„Фауна Србије”„Српске шуме на издисају”„Lepih šest odsto Srbije”„Илустрована историја Срба — Увод”„Винчанска култура - Градска општина Гроцка”„''„Винча — Праисторијска метропола”''”оригиналаЈужни Словени под византијском влашћу (600—1025)Држава маћедонских Словена„Карађорђе истина и мит, Проф. др Радош Љушић, Вечерње новости, фељтон, 18 наставака, 24. август - 10. септембар 2003.”„Политика: Како је утврђена војна неутралност, 13. јануар. 2010, приступљено децембра 2012.”„Србија и РС оживеле Дејтонски споразум”„Са српским пасошем у 104 земље”Војска Србије | О Војсци | Војска Србије — Улога, намена и задациАрхивираноВојска Србије | ОрганизацијаАрхивираноОдлука о изради Стратегије просторног развоја Републике Србије до 2020. годинеЗакон о територијалној организацији Републике СрбијеЗакон о државној управиНајчешће постављана питања.„Смањење броја статистичких региона кроз измене Закона о регионалном развоју”„2011 Human development Report”„Službena upotreba jezika i pisama”„Попис становништва, домаћинстава и станова 2011. године у Републици Србији. Књига 4: Вероисповест, матерњи језик и национална припадност”„Вероисповест, матерњи језик и национална”„Специјална известитељка УН за слободу религије и вероисповести Асма Јахангир, код Заштитника грађана Саше Јанковића”„Закон о државним и другим празницима у Републици Србији”„Веронаука у српским школама”„Serbia – Ancestral Genography Atlas”Бела књига Милошевићеве владавинеоригиналаGross domestic product based on purchasing-power-parity (PPP) per capita GDP БДП 2007—2013Актуелни показатељи — Република Србија„Попис становништва, домаћинстава и станова 2011. године у Републици Србији Књига 7: Економска активност”Zemlje kandidati za članstvo u EU„Putin drops South Stream gas pipeline to EU, courts Turkey”„„Соко — историјат””оригинала„„Рембас — историјат””оригинала„„Лубница — историјат””оригинала„„Штаваљ — Историјат””оригинала„„Боговина — историјат””оригинала„„Јасеновац — историјат””оригинала„„Вршка чука — историјат””оригинала„„Ибарски рудници — историјат””оригинала„Закон о просторном плану Републике Србије од 2010 до 2020”„Кривични законик — Недозвољена изградња нуклеарних постројења, члан 267”„Б92: Srbija uklonila obogaćeni uranijum, 25. октобар 2011”„Коришћење енергије ветра у Србији — природни услови и практична примена”„Енергија ветра”„Србија може да прави струју од сунца, биомасе, воде и ветра”„Моја електрана и друге ветрењаче”„Биомаса, струја без инвестиција”„Auto-karte Srbije”„www.srbija.gov.rs Статистике о Србији”оригинала„Статистика зе месец децембар и 2016. годину”„Turizam u Srbiji”„Univerzitet u Beogradu: Vek i po akademskog znanja”„Vojnomedicinska akademija: 165 godina tradicije i napretka”Никола Гиљен, Соња Јовићевић Јов и Јелена Мандић: Мирослављево јеванђеље; Текст је публикован у ревији „Историја” и настао је као део научно-истраживачког рада Фонда „Принцеза Оливера”„World music асоцијација Србије”оригинала„World music у Србији”оригинала„Pogledajte: Boban Marković svira u redakciji „Blica”!”„Eurovision Song Contest 2007 Final”„Projekat Rastko, Alojz Ujes: Joakim Vujic”„Унеско”„Списак локалитета Светске баштине”„Guča i Egzit zaludeli svet”оригинала„Sabor trubača GUČA”„Interesting facts about Exit”оригинала„FIFA Association Information”„Serbia women win EuroBasket title, gain first Olympics berth”„Odbojkašice ispisale istoriju – Srbija je svetski prvak!”„Сајт Ватерполо савеза Србије, Освојене медаље”„Сајт ФК Црвена звезда, Бари”„Сајт ФК Црвена звезда, Токио”„Blic:Zlatna Milica! Mandićeva donela Srbiji najsjajnije odličje u Londonu!”„Милица Мандић освојила златну медаљу („Политика”, 12. август 2012)”„Златни Давор Штефанек”„DŽUDO ŠAMPIONAT Majdov osvojio svetsko zlato”„Španovićeva trećim skokom svih vremena do zlata!”„Чудо Иване Шпановић — 7,24 м („Политика”, 5. март 2017)”The Age of Nepotism: Travel Journals and Observations from the Balkans During the DepressionCalcium and Magnesium in Groundwater: Occurrence and Significance for Human HealthComparative Hungarian Cultural StudiesБела књига Милошевићеве владавинеоригиналаComparative Hungarian Cultural StudiesSabres of Two Easts: An Untold History of Muslims in Eastern Europe, Their Friends and FoesГеографија за осми разред основне школеSerbia: the country, people, life, customsМедијиВодичПодациВлада Републике СрбијеНародна скупштина Републике СрбијеНародна канцеларија председника Републике СрбијеНародна банка СрбијеТуристичка организација СрбијеПортал еУправе Републике СрбијеРепубличко јавно правобранилаштвоууууууWorldCat151202876n851959190000 0000 9526 67094054598-24101000570825ge130919