Find $lambda^{d}(A_{d}(a))$ and determine its behaviour as $d to infty$












0












$begingroup$


Set $A_{d}(a):={(x_{1},...,x_{d})inmathbb [0,infty[^{d}: sum_{i=1}^{d}x_{i}leq a}$, whereby $a > 0$



Determine:



(i) $lambda^{d}(A_{d}(a))$



(ii) how $(A_{d}(1))$ behaves as $d to infty$



Is there a formula for n-dimensional squares? (At least I think it is a square).










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$endgroup$








  • 1




    $begingroup$
    This is not a sphere: draw it for $d=2$!
    $endgroup$
    – Mindlack
    Jan 8 at 16:07










  • $begingroup$
    It would be a square, correct?
    $endgroup$
    – MinaThuma
    Jan 8 at 16:25










  • $begingroup$
    No, it is not a square.
    $endgroup$
    – Mindlack
    Jan 8 at 17:12










  • $begingroup$
    Well then diamond-like
    $endgroup$
    – MinaThuma
    Jan 8 at 17:24










  • $begingroup$
    No: negative values are forbidden!
    $endgroup$
    – Mindlack
    Jan 8 at 17:27
















0












$begingroup$


Set $A_{d}(a):={(x_{1},...,x_{d})inmathbb [0,infty[^{d}: sum_{i=1}^{d}x_{i}leq a}$, whereby $a > 0$



Determine:



(i) $lambda^{d}(A_{d}(a))$



(ii) how $(A_{d}(1))$ behaves as $d to infty$



Is there a formula for n-dimensional squares? (At least I think it is a square).










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    This is not a sphere: draw it for $d=2$!
    $endgroup$
    – Mindlack
    Jan 8 at 16:07










  • $begingroup$
    It would be a square, correct?
    $endgroup$
    – MinaThuma
    Jan 8 at 16:25










  • $begingroup$
    No, it is not a square.
    $endgroup$
    – Mindlack
    Jan 8 at 17:12










  • $begingroup$
    Well then diamond-like
    $endgroup$
    – MinaThuma
    Jan 8 at 17:24










  • $begingroup$
    No: negative values are forbidden!
    $endgroup$
    – Mindlack
    Jan 8 at 17:27














0












0








0





$begingroup$


Set $A_{d}(a):={(x_{1},...,x_{d})inmathbb [0,infty[^{d}: sum_{i=1}^{d}x_{i}leq a}$, whereby $a > 0$



Determine:



(i) $lambda^{d}(A_{d}(a))$



(ii) how $(A_{d}(1))$ behaves as $d to infty$



Is there a formula for n-dimensional squares? (At least I think it is a square).










share|cite|improve this question











$endgroup$




Set $A_{d}(a):={(x_{1},...,x_{d})inmathbb [0,infty[^{d}: sum_{i=1}^{d}x_{i}leq a}$, whereby $a > 0$



Determine:



(i) $lambda^{d}(A_{d}(a))$



(ii) how $(A_{d}(1))$ behaves as $d to infty$



Is there a formula for n-dimensional squares? (At least I think it is a square).







real-analysis measure-theory lebesgue-integral volume






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Jan 8 at 16:13







MinaThuma

















asked Jan 8 at 15:59









MinaThumaMinaThuma

798




798








  • 1




    $begingroup$
    This is not a sphere: draw it for $d=2$!
    $endgroup$
    – Mindlack
    Jan 8 at 16:07










  • $begingroup$
    It would be a square, correct?
    $endgroup$
    – MinaThuma
    Jan 8 at 16:25










  • $begingroup$
    No, it is not a square.
    $endgroup$
    – Mindlack
    Jan 8 at 17:12










  • $begingroup$
    Well then diamond-like
    $endgroup$
    – MinaThuma
    Jan 8 at 17:24










  • $begingroup$
    No: negative values are forbidden!
    $endgroup$
    – Mindlack
    Jan 8 at 17:27














  • 1




    $begingroup$
    This is not a sphere: draw it for $d=2$!
    $endgroup$
    – Mindlack
    Jan 8 at 16:07










  • $begingroup$
    It would be a square, correct?
    $endgroup$
    – MinaThuma
    Jan 8 at 16:25










  • $begingroup$
    No, it is not a square.
    $endgroup$
    – Mindlack
    Jan 8 at 17:12










  • $begingroup$
    Well then diamond-like
    $endgroup$
    – MinaThuma
    Jan 8 at 17:24










  • $begingroup$
    No: negative values are forbidden!
    $endgroup$
    – Mindlack
    Jan 8 at 17:27








1




1




$begingroup$
This is not a sphere: draw it for $d=2$!
$endgroup$
– Mindlack
Jan 8 at 16:07




$begingroup$
This is not a sphere: draw it for $d=2$!
$endgroup$
– Mindlack
Jan 8 at 16:07












$begingroup$
It would be a square, correct?
$endgroup$
– MinaThuma
Jan 8 at 16:25




$begingroup$
It would be a square, correct?
$endgroup$
– MinaThuma
Jan 8 at 16:25












$begingroup$
No, it is not a square.
$endgroup$
– Mindlack
Jan 8 at 17:12




$begingroup$
No, it is not a square.
$endgroup$
– Mindlack
Jan 8 at 17:12












$begingroup$
Well then diamond-like
$endgroup$
– MinaThuma
Jan 8 at 17:24




$begingroup$
Well then diamond-like
$endgroup$
– MinaThuma
Jan 8 at 17:24












$begingroup$
No: negative values are forbidden!
$endgroup$
– Mindlack
Jan 8 at 17:27




$begingroup$
No: negative values are forbidden!
$endgroup$
– Mindlack
Jan 8 at 17:27










1 Answer
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oldest

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1












$begingroup$

You can evaluate the volume as an iterated integral.



Since $x_1 + cdots + x_d le a$ a point $x = (x_1,ldots,x_d)$ belongs to the region $A_d(a)$ if and only if




  • $ 0 le x_1 le a$

  • $ 0 le x_2 le a - x_1$

  • $0 le x_3 le a - x_1 - x_2$


and so on until you get to





  • $0 le x_d le a - x_1 - cdots - x_{d-1}$.


The elementary $d$-volume of $A_d(a)$ satisfies
$$V_d(A_d(a)) = int_0^a int_0^{a - x_1} int_0^{a - x_1 - x_2} cdots int_0^{a - x_1 - cdots - x_{d-1}} , dx_d dx_{d-1} cdots dx_1.$$



You could try to work this out directly, or look for a pattern and formulate a proof by induction. It isn't hard to see that




  • $V_1(A_1(a)) = a$

  • $V_2(A_2(a)) = dfrac{a^2}{2}$

  • $V_3(A_3(a)) = dfrac{a^3}{6}$


so one might have the audacity to conjecture that $V_d(A_d(a)) = dfrac{a^d}{d!}$.



Since the cases $d=1$ through $d=3$ have been dispensed with it remains only to make the induction step. Assuming that the formula holds for $d-1$, a close look at the integral defining $V_d(A_d(a))$ shows
$$V_d(A_d(a)) = int_0^a V_{d-1}(A_{d-1}(a - x_1)) , dx_1 = int_0^a frac{(a-x_1)^{d-1}}{(d-1)!} , dx_1 = frac{a^d}{d!}.$$






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    $begingroup$

    You can evaluate the volume as an iterated integral.



    Since $x_1 + cdots + x_d le a$ a point $x = (x_1,ldots,x_d)$ belongs to the region $A_d(a)$ if and only if




    • $ 0 le x_1 le a$

    • $ 0 le x_2 le a - x_1$

    • $0 le x_3 le a - x_1 - x_2$


    and so on until you get to





    • $0 le x_d le a - x_1 - cdots - x_{d-1}$.


    The elementary $d$-volume of $A_d(a)$ satisfies
    $$V_d(A_d(a)) = int_0^a int_0^{a - x_1} int_0^{a - x_1 - x_2} cdots int_0^{a - x_1 - cdots - x_{d-1}} , dx_d dx_{d-1} cdots dx_1.$$



    You could try to work this out directly, or look for a pattern and formulate a proof by induction. It isn't hard to see that




    • $V_1(A_1(a)) = a$

    • $V_2(A_2(a)) = dfrac{a^2}{2}$

    • $V_3(A_3(a)) = dfrac{a^3}{6}$


    so one might have the audacity to conjecture that $V_d(A_d(a)) = dfrac{a^d}{d!}$.



    Since the cases $d=1$ through $d=3$ have been dispensed with it remains only to make the induction step. Assuming that the formula holds for $d-1$, a close look at the integral defining $V_d(A_d(a))$ shows
    $$V_d(A_d(a)) = int_0^a V_{d-1}(A_{d-1}(a - x_1)) , dx_1 = int_0^a frac{(a-x_1)^{d-1}}{(d-1)!} , dx_1 = frac{a^d}{d!}.$$






    share|cite|improve this answer









    $endgroup$


















      1












      $begingroup$

      You can evaluate the volume as an iterated integral.



      Since $x_1 + cdots + x_d le a$ a point $x = (x_1,ldots,x_d)$ belongs to the region $A_d(a)$ if and only if




      • $ 0 le x_1 le a$

      • $ 0 le x_2 le a - x_1$

      • $0 le x_3 le a - x_1 - x_2$


      and so on until you get to





      • $0 le x_d le a - x_1 - cdots - x_{d-1}$.


      The elementary $d$-volume of $A_d(a)$ satisfies
      $$V_d(A_d(a)) = int_0^a int_0^{a - x_1} int_0^{a - x_1 - x_2} cdots int_0^{a - x_1 - cdots - x_{d-1}} , dx_d dx_{d-1} cdots dx_1.$$



      You could try to work this out directly, or look for a pattern and formulate a proof by induction. It isn't hard to see that




      • $V_1(A_1(a)) = a$

      • $V_2(A_2(a)) = dfrac{a^2}{2}$

      • $V_3(A_3(a)) = dfrac{a^3}{6}$


      so one might have the audacity to conjecture that $V_d(A_d(a)) = dfrac{a^d}{d!}$.



      Since the cases $d=1$ through $d=3$ have been dispensed with it remains only to make the induction step. Assuming that the formula holds for $d-1$, a close look at the integral defining $V_d(A_d(a))$ shows
      $$V_d(A_d(a)) = int_0^a V_{d-1}(A_{d-1}(a - x_1)) , dx_1 = int_0^a frac{(a-x_1)^{d-1}}{(d-1)!} , dx_1 = frac{a^d}{d!}.$$






      share|cite|improve this answer









      $endgroup$
















        1












        1








        1





        $begingroup$

        You can evaluate the volume as an iterated integral.



        Since $x_1 + cdots + x_d le a$ a point $x = (x_1,ldots,x_d)$ belongs to the region $A_d(a)$ if and only if




        • $ 0 le x_1 le a$

        • $ 0 le x_2 le a - x_1$

        • $0 le x_3 le a - x_1 - x_2$


        and so on until you get to





        • $0 le x_d le a - x_1 - cdots - x_{d-1}$.


        The elementary $d$-volume of $A_d(a)$ satisfies
        $$V_d(A_d(a)) = int_0^a int_0^{a - x_1} int_0^{a - x_1 - x_2} cdots int_0^{a - x_1 - cdots - x_{d-1}} , dx_d dx_{d-1} cdots dx_1.$$



        You could try to work this out directly, or look for a pattern and formulate a proof by induction. It isn't hard to see that




        • $V_1(A_1(a)) = a$

        • $V_2(A_2(a)) = dfrac{a^2}{2}$

        • $V_3(A_3(a)) = dfrac{a^3}{6}$


        so one might have the audacity to conjecture that $V_d(A_d(a)) = dfrac{a^d}{d!}$.



        Since the cases $d=1$ through $d=3$ have been dispensed with it remains only to make the induction step. Assuming that the formula holds for $d-1$, a close look at the integral defining $V_d(A_d(a))$ shows
        $$V_d(A_d(a)) = int_0^a V_{d-1}(A_{d-1}(a - x_1)) , dx_1 = int_0^a frac{(a-x_1)^{d-1}}{(d-1)!} , dx_1 = frac{a^d}{d!}.$$






        share|cite|improve this answer









        $endgroup$



        You can evaluate the volume as an iterated integral.



        Since $x_1 + cdots + x_d le a$ a point $x = (x_1,ldots,x_d)$ belongs to the region $A_d(a)$ if and only if




        • $ 0 le x_1 le a$

        • $ 0 le x_2 le a - x_1$

        • $0 le x_3 le a - x_1 - x_2$


        and so on until you get to





        • $0 le x_d le a - x_1 - cdots - x_{d-1}$.


        The elementary $d$-volume of $A_d(a)$ satisfies
        $$V_d(A_d(a)) = int_0^a int_0^{a - x_1} int_0^{a - x_1 - x_2} cdots int_0^{a - x_1 - cdots - x_{d-1}} , dx_d dx_{d-1} cdots dx_1.$$



        You could try to work this out directly, or look for a pattern and formulate a proof by induction. It isn't hard to see that




        • $V_1(A_1(a)) = a$

        • $V_2(A_2(a)) = dfrac{a^2}{2}$

        • $V_3(A_3(a)) = dfrac{a^3}{6}$


        so one might have the audacity to conjecture that $V_d(A_d(a)) = dfrac{a^d}{d!}$.



        Since the cases $d=1$ through $d=3$ have been dispensed with it remains only to make the induction step. Assuming that the formula holds for $d-1$, a close look at the integral defining $V_d(A_d(a))$ shows
        $$V_d(A_d(a)) = int_0^a V_{d-1}(A_{d-1}(a - x_1)) , dx_1 = int_0^a frac{(a-x_1)^{d-1}}{(d-1)!} , dx_1 = frac{a^d}{d!}.$$







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Jan 8 at 21:25









        Umberto P.Umberto P.

        39k13064




        39k13064






























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