Limit of $left{ int_{0}^{1} [bx + a(1 - x) ]^{frac1n} dx right}^n$ as $n to infty$












5















Evaluate the limit for $0 < a < b$,
$$lim_{n to infty} left{ int_{0}^{1} [bx + a(1 - x) ]^{frac1n} dx right}^n$$




Just to be clear, the exponent $~1/n~$ is inside the integration on the entire integrand $~a + (b-a)x,~$ and the exponent $n$ is outside on the definite integral.



I actually have been able to solve it as I happen to know a particular way of viewing the logarithm function as a limit
$$log x = lim_{h to 0} frac{x^h - 1}h quad text{, or equivalently} quadlog x = lim_{n to infty} n(x^{frac1n} - 1)$$



That is, my solution is a process that involves terms like $~e^{blog b},~$ where I have to obtain $~log b~$ first as a limit, and I can say that it is $~b^b~$ at the very last step only after another limit.




My question is this: how do I evaluate the limit more directly without this seemingly redundant path of log on the exponent?




In short, I have a solution which I don't like, and I believe there are better ones.



Any ideas? Thank you.





As a reference, below is the detailed steps of my circuitous solution:



The definite integral evaluates to
$$frac1{b - a} frac1{ 1 + frac1n } left[ a + (b-a)x right]^{ 1 + frac1n } Bigg|_{0}^{1} = frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n }$$
Thus the whole expression becomes
$$
begin{align}
&lim_{n to infty} left{ frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n } right}^{n} \
&= frac1e lim_{n to infty} left{ 1 + frac{ b^{1 + frac1n} - a^{1 + frac1n} - (b - a) }{b - a} right}^{n} \
&= frac1e lim_{n to infty} left{ 1 + frac{ n left( b^{1 + frac1n} - b right) - n left(
a^{1 + frac1n} - a right) }{ n (b - a) } right}^{n}
end{align}
$$
all the limits exist so I'm just gonna keep writing in this non-rigorous way
$$
begin{align}
&= frac1e lim_{n to infty} left{ 1 + frac1n frac{ b log b - a log a }{ b - a } right}^{n} \
&= frac1e cdot e^{ frac1{b-a} left( b log b - a log a right)} \
&= frac1e left( frac{ b^b }{ a^a } right)^{ frac1{b-a}}
end{align}$$










share|cite|improve this question





























    5















    Evaluate the limit for $0 < a < b$,
    $$lim_{n to infty} left{ int_{0}^{1} [bx + a(1 - x) ]^{frac1n} dx right}^n$$




    Just to be clear, the exponent $~1/n~$ is inside the integration on the entire integrand $~a + (b-a)x,~$ and the exponent $n$ is outside on the definite integral.



    I actually have been able to solve it as I happen to know a particular way of viewing the logarithm function as a limit
    $$log x = lim_{h to 0} frac{x^h - 1}h quad text{, or equivalently} quadlog x = lim_{n to infty} n(x^{frac1n} - 1)$$



    That is, my solution is a process that involves terms like $~e^{blog b},~$ where I have to obtain $~log b~$ first as a limit, and I can say that it is $~b^b~$ at the very last step only after another limit.




    My question is this: how do I evaluate the limit more directly without this seemingly redundant path of log on the exponent?




    In short, I have a solution which I don't like, and I believe there are better ones.



    Any ideas? Thank you.





    As a reference, below is the detailed steps of my circuitous solution:



    The definite integral evaluates to
    $$frac1{b - a} frac1{ 1 + frac1n } left[ a + (b-a)x right]^{ 1 + frac1n } Bigg|_{0}^{1} = frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n }$$
    Thus the whole expression becomes
    $$
    begin{align}
    &lim_{n to infty} left{ frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n } right}^{n} \
    &= frac1e lim_{n to infty} left{ 1 + frac{ b^{1 + frac1n} - a^{1 + frac1n} - (b - a) }{b - a} right}^{n} \
    &= frac1e lim_{n to infty} left{ 1 + frac{ n left( b^{1 + frac1n} - b right) - n left(
    a^{1 + frac1n} - a right) }{ n (b - a) } right}^{n}
    end{align}
    $$
    all the limits exist so I'm just gonna keep writing in this non-rigorous way
    $$
    begin{align}
    &= frac1e lim_{n to infty} left{ 1 + frac1n frac{ b log b - a log a }{ b - a } right}^{n} \
    &= frac1e cdot e^{ frac1{b-a} left( b log b - a log a right)} \
    &= frac1e left( frac{ b^b }{ a^a } right)^{ frac1{b-a}}
    end{align}$$










    share|cite|improve this question



























      5












      5








      5


      2






      Evaluate the limit for $0 < a < b$,
      $$lim_{n to infty} left{ int_{0}^{1} [bx + a(1 - x) ]^{frac1n} dx right}^n$$




      Just to be clear, the exponent $~1/n~$ is inside the integration on the entire integrand $~a + (b-a)x,~$ and the exponent $n$ is outside on the definite integral.



      I actually have been able to solve it as I happen to know a particular way of viewing the logarithm function as a limit
      $$log x = lim_{h to 0} frac{x^h - 1}h quad text{, or equivalently} quadlog x = lim_{n to infty} n(x^{frac1n} - 1)$$



      That is, my solution is a process that involves terms like $~e^{blog b},~$ where I have to obtain $~log b~$ first as a limit, and I can say that it is $~b^b~$ at the very last step only after another limit.




      My question is this: how do I evaluate the limit more directly without this seemingly redundant path of log on the exponent?




      In short, I have a solution which I don't like, and I believe there are better ones.



      Any ideas? Thank you.





      As a reference, below is the detailed steps of my circuitous solution:



      The definite integral evaluates to
      $$frac1{b - a} frac1{ 1 + frac1n } left[ a + (b-a)x right]^{ 1 + frac1n } Bigg|_{0}^{1} = frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n }$$
      Thus the whole expression becomes
      $$
      begin{align}
      &lim_{n to infty} left{ frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n } right}^{n} \
      &= frac1e lim_{n to infty} left{ 1 + frac{ b^{1 + frac1n} - a^{1 + frac1n} - (b - a) }{b - a} right}^{n} \
      &= frac1e lim_{n to infty} left{ 1 + frac{ n left( b^{1 + frac1n} - b right) - n left(
      a^{1 + frac1n} - a right) }{ n (b - a) } right}^{n}
      end{align}
      $$
      all the limits exist so I'm just gonna keep writing in this non-rigorous way
      $$
      begin{align}
      &= frac1e lim_{n to infty} left{ 1 + frac1n frac{ b log b - a log a }{ b - a } right}^{n} \
      &= frac1e cdot e^{ frac1{b-a} left( b log b - a log a right)} \
      &= frac1e left( frac{ b^b }{ a^a } right)^{ frac1{b-a}}
      end{align}$$










      share|cite|improve this question
















      Evaluate the limit for $0 < a < b$,
      $$lim_{n to infty} left{ int_{0}^{1} [bx + a(1 - x) ]^{frac1n} dx right}^n$$




      Just to be clear, the exponent $~1/n~$ is inside the integration on the entire integrand $~a + (b-a)x,~$ and the exponent $n$ is outside on the definite integral.



      I actually have been able to solve it as I happen to know a particular way of viewing the logarithm function as a limit
      $$log x = lim_{h to 0} frac{x^h - 1}h quad text{, or equivalently} quadlog x = lim_{n to infty} n(x^{frac1n} - 1)$$



      That is, my solution is a process that involves terms like $~e^{blog b},~$ where I have to obtain $~log b~$ first as a limit, and I can say that it is $~b^b~$ at the very last step only after another limit.




      My question is this: how do I evaluate the limit more directly without this seemingly redundant path of log on the exponent?




      In short, I have a solution which I don't like, and I believe there are better ones.



      Any ideas? Thank you.





      As a reference, below is the detailed steps of my circuitous solution:



      The definite integral evaluates to
      $$frac1{b - a} frac1{ 1 + frac1n } left[ a + (b-a)x right]^{ 1 + frac1n } Bigg|_{0}^{1} = frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n }$$
      Thus the whole expression becomes
      $$
      begin{align}
      &lim_{n to infty} left{ frac{ b^{1 + frac1n} - a^{1 + frac1n} }{b - a} frac1{ 1 + frac1n } right}^{n} \
      &= frac1e lim_{n to infty} left{ 1 + frac{ b^{1 + frac1n} - a^{1 + frac1n} - (b - a) }{b - a} right}^{n} \
      &= frac1e lim_{n to infty} left{ 1 + frac{ n left( b^{1 + frac1n} - b right) - n left(
      a^{1 + frac1n} - a right) }{ n (b - a) } right}^{n}
      end{align}
      $$
      all the limits exist so I'm just gonna keep writing in this non-rigorous way
      $$
      begin{align}
      &= frac1e lim_{n to infty} left{ 1 + frac1n frac{ b log b - a log a }{ b - a } right}^{n} \
      &= frac1e cdot e^{ frac1{b-a} left( b log b - a log a right)} \
      &= frac1e left( frac{ b^b }{ a^a } right)^{ frac1{b-a}}
      end{align}$$







      calculus limits alternative-proof






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      edited Dec 10 '18 at 17:34

























      asked Oct 19 '16 at 15:01









      Lee David Chung Lin

      3,74531140




      3,74531140






















          2 Answers
          2






          active

          oldest

          votes


















          5














          This is just the continuous analogue of a well-known fact:




          If $a_1,a_2,ldots,a_m$ are non-negative numbers and the mean of order $p>0$ is defined as
          $$ M_p(a_1,ldots,a_m) = left(frac{1}{m}sum_{k=1}^{m}a_k^pright)^{frac{1}{p}},$$
          then $M_p$ is an increasing function of $p$ and
          $$ lim_{pto 0^+} M_p(a_1,ldots,a_m)= GM(a_1,ldots,a_m) = left(prod_{k=1}^{m}a_kright)^{frac{1}{m}}$$
          by the continuity and concavity of the logarithm function.




          In particular, if $f(x)$ is a non-negative and continuous function over the interval $(0,1)$,




          $$ lim_{pto 0^+}left(int_{0}^{1}f(x)^p,dxright)^{frac{1}{p}}=expint_{0}^{1}log f(x),dx.$$




          The last identity gives that for any $a,b>0$,



          $$ begin{eqnarray*}lim_{nto +infty}left(int_{0}^{1}(bx+a(1-x))^{frac{1}{n}},dxright)^n &=& expint_{0}^{1}log(bx+a(1-x)),dx\&=&expleft[frac{1}{b-a}int_{a}^{b}log(x),dxright]\&=&expleft[-1+frac{blog b-alog a}{b-a}right]\&=&color{red}{frac{1}{e}left(frac{b^b}{a^a}right)^{frac{1}{b-a}}} end{eqnarray*}$$
          as claimed.






          share|cite|improve this answer

















          • 2




            Putting it in this bigger framework is really great!
            – Lee David Chung Lin
            Oct 19 '16 at 16:17






          • 1




            This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
            – Brevan Ellefsen
            Oct 20 '16 at 2:47



















          5














          $newcommand{bbx}[1]{,bbox[8px,border:1px groove navy]{{#1}},}
          newcommand{braces}[1]{leftlbrace,{#1},rightrbrace}
          newcommand{bracks}[1]{leftlbrack,{#1},rightrbrack}
          newcommand{dd}{mathrm{d}}
          newcommand{ds}[1]{displaystyle{#1}}
          newcommand{expo}[1]{,mathrm{e}^{#1},}
          newcommand{ic}{mathrm{i}}
          newcommand{mc}[1]{mathcal{#1}}
          newcommand{mrm}[1]{mathrm{#1}}
          newcommand{pars}[1]{left(,{#1},right)}
          newcommand{partiald}[3]{frac{partial^{#1} #2}{partial #3^{#1}}}
          newcommand{root}[2]{,sqrt[#1]{,{#2},},}
          newcommand{totald}[3]{frac{mathrm{d}^{#1} #2}{mathrm{d} #3^{#1}}}
          newcommand{verts}[1]{leftvert,{#1},rightvert}$
          begin{align}
          &lim_{n to infty}braces{int_{0}^{1}bracks{bx + apars{1 - x}}^{1/n}
          ,dd x}^{n} =
          lim_{n to infty}bracks{{1 over b - a}int_{a}^{b}x^{1/n}
          ,dd x}^{n}
          \[5mm] &=
          lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} + lnpars{int_{a}^{b}x^{epsilon},dd x} over epsilon}
          \[5mm] & =
          lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} +
          lnpars{b^{epsilon + 1} - a^{epsilon + 1}} - lnpars{epsilon + 1} over epsilon}
          \[5mm] & =
          lim_{epsilon to 0^{+}}exppars{
          {b^{epsilon + 1}lnpars{b} - a^{epsilon + 1}lnpars{a} over b^{epsilon + 1} - a^{epsilon + 1}} - {1 over epsilon + 1}}qquadqquad
          pars{~L'Hhat{o}pital Rule~}
          \[5mm] & =
          exppars{{blnpars{b} - alnpars{a} over b - a} - 1} =
          bbx{ds{{1 over expo{}},pars{b^{b} over a^{a}}^{1/pars{b - a}}}}
          end{align}






          share|cite|improve this answer





















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            2 Answers
            2






            active

            oldest

            votes








            2 Answers
            2






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes









            5














            This is just the continuous analogue of a well-known fact:




            If $a_1,a_2,ldots,a_m$ are non-negative numbers and the mean of order $p>0$ is defined as
            $$ M_p(a_1,ldots,a_m) = left(frac{1}{m}sum_{k=1}^{m}a_k^pright)^{frac{1}{p}},$$
            then $M_p$ is an increasing function of $p$ and
            $$ lim_{pto 0^+} M_p(a_1,ldots,a_m)= GM(a_1,ldots,a_m) = left(prod_{k=1}^{m}a_kright)^{frac{1}{m}}$$
            by the continuity and concavity of the logarithm function.




            In particular, if $f(x)$ is a non-negative and continuous function over the interval $(0,1)$,




            $$ lim_{pto 0^+}left(int_{0}^{1}f(x)^p,dxright)^{frac{1}{p}}=expint_{0}^{1}log f(x),dx.$$




            The last identity gives that for any $a,b>0$,



            $$ begin{eqnarray*}lim_{nto +infty}left(int_{0}^{1}(bx+a(1-x))^{frac{1}{n}},dxright)^n &=& expint_{0}^{1}log(bx+a(1-x)),dx\&=&expleft[frac{1}{b-a}int_{a}^{b}log(x),dxright]\&=&expleft[-1+frac{blog b-alog a}{b-a}right]\&=&color{red}{frac{1}{e}left(frac{b^b}{a^a}right)^{frac{1}{b-a}}} end{eqnarray*}$$
            as claimed.






            share|cite|improve this answer

















            • 2




              Putting it in this bigger framework is really great!
              – Lee David Chung Lin
              Oct 19 '16 at 16:17






            • 1




              This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
              – Brevan Ellefsen
              Oct 20 '16 at 2:47
















            5














            This is just the continuous analogue of a well-known fact:




            If $a_1,a_2,ldots,a_m$ are non-negative numbers and the mean of order $p>0$ is defined as
            $$ M_p(a_1,ldots,a_m) = left(frac{1}{m}sum_{k=1}^{m}a_k^pright)^{frac{1}{p}},$$
            then $M_p$ is an increasing function of $p$ and
            $$ lim_{pto 0^+} M_p(a_1,ldots,a_m)= GM(a_1,ldots,a_m) = left(prod_{k=1}^{m}a_kright)^{frac{1}{m}}$$
            by the continuity and concavity of the logarithm function.




            In particular, if $f(x)$ is a non-negative and continuous function over the interval $(0,1)$,




            $$ lim_{pto 0^+}left(int_{0}^{1}f(x)^p,dxright)^{frac{1}{p}}=expint_{0}^{1}log f(x),dx.$$




            The last identity gives that for any $a,b>0$,



            $$ begin{eqnarray*}lim_{nto +infty}left(int_{0}^{1}(bx+a(1-x))^{frac{1}{n}},dxright)^n &=& expint_{0}^{1}log(bx+a(1-x)),dx\&=&expleft[frac{1}{b-a}int_{a}^{b}log(x),dxright]\&=&expleft[-1+frac{blog b-alog a}{b-a}right]\&=&color{red}{frac{1}{e}left(frac{b^b}{a^a}right)^{frac{1}{b-a}}} end{eqnarray*}$$
            as claimed.






            share|cite|improve this answer

















            • 2




              Putting it in this bigger framework is really great!
              – Lee David Chung Lin
              Oct 19 '16 at 16:17






            • 1




              This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
              – Brevan Ellefsen
              Oct 20 '16 at 2:47














            5












            5








            5






            This is just the continuous analogue of a well-known fact:




            If $a_1,a_2,ldots,a_m$ are non-negative numbers and the mean of order $p>0$ is defined as
            $$ M_p(a_1,ldots,a_m) = left(frac{1}{m}sum_{k=1}^{m}a_k^pright)^{frac{1}{p}},$$
            then $M_p$ is an increasing function of $p$ and
            $$ lim_{pto 0^+} M_p(a_1,ldots,a_m)= GM(a_1,ldots,a_m) = left(prod_{k=1}^{m}a_kright)^{frac{1}{m}}$$
            by the continuity and concavity of the logarithm function.




            In particular, if $f(x)$ is a non-negative and continuous function over the interval $(0,1)$,




            $$ lim_{pto 0^+}left(int_{0}^{1}f(x)^p,dxright)^{frac{1}{p}}=expint_{0}^{1}log f(x),dx.$$




            The last identity gives that for any $a,b>0$,



            $$ begin{eqnarray*}lim_{nto +infty}left(int_{0}^{1}(bx+a(1-x))^{frac{1}{n}},dxright)^n &=& expint_{0}^{1}log(bx+a(1-x)),dx\&=&expleft[frac{1}{b-a}int_{a}^{b}log(x),dxright]\&=&expleft[-1+frac{blog b-alog a}{b-a}right]\&=&color{red}{frac{1}{e}left(frac{b^b}{a^a}right)^{frac{1}{b-a}}} end{eqnarray*}$$
            as claimed.






            share|cite|improve this answer












            This is just the continuous analogue of a well-known fact:




            If $a_1,a_2,ldots,a_m$ are non-negative numbers and the mean of order $p>0$ is defined as
            $$ M_p(a_1,ldots,a_m) = left(frac{1}{m}sum_{k=1}^{m}a_k^pright)^{frac{1}{p}},$$
            then $M_p$ is an increasing function of $p$ and
            $$ lim_{pto 0^+} M_p(a_1,ldots,a_m)= GM(a_1,ldots,a_m) = left(prod_{k=1}^{m}a_kright)^{frac{1}{m}}$$
            by the continuity and concavity of the logarithm function.




            In particular, if $f(x)$ is a non-negative and continuous function over the interval $(0,1)$,




            $$ lim_{pto 0^+}left(int_{0}^{1}f(x)^p,dxright)^{frac{1}{p}}=expint_{0}^{1}log f(x),dx.$$




            The last identity gives that for any $a,b>0$,



            $$ begin{eqnarray*}lim_{nto +infty}left(int_{0}^{1}(bx+a(1-x))^{frac{1}{n}},dxright)^n &=& expint_{0}^{1}log(bx+a(1-x)),dx\&=&expleft[frac{1}{b-a}int_{a}^{b}log(x),dxright]\&=&expleft[-1+frac{blog b-alog a}{b-a}right]\&=&color{red}{frac{1}{e}left(frac{b^b}{a^a}right)^{frac{1}{b-a}}} end{eqnarray*}$$
            as claimed.







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Oct 19 '16 at 16:08









            Jack D'Aurizio

            287k33280657




            287k33280657








            • 2




              Putting it in this bigger framework is really great!
              – Lee David Chung Lin
              Oct 19 '16 at 16:17






            • 1




              This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
              – Brevan Ellefsen
              Oct 20 '16 at 2:47














            • 2




              Putting it in this bigger framework is really great!
              – Lee David Chung Lin
              Oct 19 '16 at 16:17






            • 1




              This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
              – Brevan Ellefsen
              Oct 20 '16 at 2:47








            2




            2




            Putting it in this bigger framework is really great!
            – Lee David Chung Lin
            Oct 19 '16 at 16:17




            Putting it in this bigger framework is really great!
            – Lee David Chung Lin
            Oct 19 '16 at 16:17




            1




            1




            This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
            – Brevan Ellefsen
            Oct 20 '16 at 2:47




            This is honestly one of the coolest things I've ever seen on Math.SE. What a wonderful theorem to know exists, and what a fascinating application. Thank you for sharing!
            – Brevan Ellefsen
            Oct 20 '16 at 2:47











            5














            $newcommand{bbx}[1]{,bbox[8px,border:1px groove navy]{{#1}},}
            newcommand{braces}[1]{leftlbrace,{#1},rightrbrace}
            newcommand{bracks}[1]{leftlbrack,{#1},rightrbrack}
            newcommand{dd}{mathrm{d}}
            newcommand{ds}[1]{displaystyle{#1}}
            newcommand{expo}[1]{,mathrm{e}^{#1},}
            newcommand{ic}{mathrm{i}}
            newcommand{mc}[1]{mathcal{#1}}
            newcommand{mrm}[1]{mathrm{#1}}
            newcommand{pars}[1]{left(,{#1},right)}
            newcommand{partiald}[3]{frac{partial^{#1} #2}{partial #3^{#1}}}
            newcommand{root}[2]{,sqrt[#1]{,{#2},},}
            newcommand{totald}[3]{frac{mathrm{d}^{#1} #2}{mathrm{d} #3^{#1}}}
            newcommand{verts}[1]{leftvert,{#1},rightvert}$
            begin{align}
            &lim_{n to infty}braces{int_{0}^{1}bracks{bx + apars{1 - x}}^{1/n}
            ,dd x}^{n} =
            lim_{n to infty}bracks{{1 over b - a}int_{a}^{b}x^{1/n}
            ,dd x}^{n}
            \[5mm] &=
            lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} + lnpars{int_{a}^{b}x^{epsilon},dd x} over epsilon}
            \[5mm] & =
            lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} +
            lnpars{b^{epsilon + 1} - a^{epsilon + 1}} - lnpars{epsilon + 1} over epsilon}
            \[5mm] & =
            lim_{epsilon to 0^{+}}exppars{
            {b^{epsilon + 1}lnpars{b} - a^{epsilon + 1}lnpars{a} over b^{epsilon + 1} - a^{epsilon + 1}} - {1 over epsilon + 1}}qquadqquad
            pars{~L'Hhat{o}pital Rule~}
            \[5mm] & =
            exppars{{blnpars{b} - alnpars{a} over b - a} - 1} =
            bbx{ds{{1 over expo{}},pars{b^{b} over a^{a}}^{1/pars{b - a}}}}
            end{align}






            share|cite|improve this answer


























              5














              $newcommand{bbx}[1]{,bbox[8px,border:1px groove navy]{{#1}},}
              newcommand{braces}[1]{leftlbrace,{#1},rightrbrace}
              newcommand{bracks}[1]{leftlbrack,{#1},rightrbrack}
              newcommand{dd}{mathrm{d}}
              newcommand{ds}[1]{displaystyle{#1}}
              newcommand{expo}[1]{,mathrm{e}^{#1},}
              newcommand{ic}{mathrm{i}}
              newcommand{mc}[1]{mathcal{#1}}
              newcommand{mrm}[1]{mathrm{#1}}
              newcommand{pars}[1]{left(,{#1},right)}
              newcommand{partiald}[3]{frac{partial^{#1} #2}{partial #3^{#1}}}
              newcommand{root}[2]{,sqrt[#1]{,{#2},},}
              newcommand{totald}[3]{frac{mathrm{d}^{#1} #2}{mathrm{d} #3^{#1}}}
              newcommand{verts}[1]{leftvert,{#1},rightvert}$
              begin{align}
              &lim_{n to infty}braces{int_{0}^{1}bracks{bx + apars{1 - x}}^{1/n}
              ,dd x}^{n} =
              lim_{n to infty}bracks{{1 over b - a}int_{a}^{b}x^{1/n}
              ,dd x}^{n}
              \[5mm] &=
              lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} + lnpars{int_{a}^{b}x^{epsilon},dd x} over epsilon}
              \[5mm] & =
              lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} +
              lnpars{b^{epsilon + 1} - a^{epsilon + 1}} - lnpars{epsilon + 1} over epsilon}
              \[5mm] & =
              lim_{epsilon to 0^{+}}exppars{
              {b^{epsilon + 1}lnpars{b} - a^{epsilon + 1}lnpars{a} over b^{epsilon + 1} - a^{epsilon + 1}} - {1 over epsilon + 1}}qquadqquad
              pars{~L'Hhat{o}pital Rule~}
              \[5mm] & =
              exppars{{blnpars{b} - alnpars{a} over b - a} - 1} =
              bbx{ds{{1 over expo{}},pars{b^{b} over a^{a}}^{1/pars{b - a}}}}
              end{align}






              share|cite|improve this answer
























                5












                5








                5






                $newcommand{bbx}[1]{,bbox[8px,border:1px groove navy]{{#1}},}
                newcommand{braces}[1]{leftlbrace,{#1},rightrbrace}
                newcommand{bracks}[1]{leftlbrack,{#1},rightrbrack}
                newcommand{dd}{mathrm{d}}
                newcommand{ds}[1]{displaystyle{#1}}
                newcommand{expo}[1]{,mathrm{e}^{#1},}
                newcommand{ic}{mathrm{i}}
                newcommand{mc}[1]{mathcal{#1}}
                newcommand{mrm}[1]{mathrm{#1}}
                newcommand{pars}[1]{left(,{#1},right)}
                newcommand{partiald}[3]{frac{partial^{#1} #2}{partial #3^{#1}}}
                newcommand{root}[2]{,sqrt[#1]{,{#2},},}
                newcommand{totald}[3]{frac{mathrm{d}^{#1} #2}{mathrm{d} #3^{#1}}}
                newcommand{verts}[1]{leftvert,{#1},rightvert}$
                begin{align}
                &lim_{n to infty}braces{int_{0}^{1}bracks{bx + apars{1 - x}}^{1/n}
                ,dd x}^{n} =
                lim_{n to infty}bracks{{1 over b - a}int_{a}^{b}x^{1/n}
                ,dd x}^{n}
                \[5mm] &=
                lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} + lnpars{int_{a}^{b}x^{epsilon},dd x} over epsilon}
                \[5mm] & =
                lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} +
                lnpars{b^{epsilon + 1} - a^{epsilon + 1}} - lnpars{epsilon + 1} over epsilon}
                \[5mm] & =
                lim_{epsilon to 0^{+}}exppars{
                {b^{epsilon + 1}lnpars{b} - a^{epsilon + 1}lnpars{a} over b^{epsilon + 1} - a^{epsilon + 1}} - {1 over epsilon + 1}}qquadqquad
                pars{~L'Hhat{o}pital Rule~}
                \[5mm] & =
                exppars{{blnpars{b} - alnpars{a} over b - a} - 1} =
                bbx{ds{{1 over expo{}},pars{b^{b} over a^{a}}^{1/pars{b - a}}}}
                end{align}






                share|cite|improve this answer












                $newcommand{bbx}[1]{,bbox[8px,border:1px groove navy]{{#1}},}
                newcommand{braces}[1]{leftlbrace,{#1},rightrbrace}
                newcommand{bracks}[1]{leftlbrack,{#1},rightrbrack}
                newcommand{dd}{mathrm{d}}
                newcommand{ds}[1]{displaystyle{#1}}
                newcommand{expo}[1]{,mathrm{e}^{#1},}
                newcommand{ic}{mathrm{i}}
                newcommand{mc}[1]{mathcal{#1}}
                newcommand{mrm}[1]{mathrm{#1}}
                newcommand{pars}[1]{left(,{#1},right)}
                newcommand{partiald}[3]{frac{partial^{#1} #2}{partial #3^{#1}}}
                newcommand{root}[2]{,sqrt[#1]{,{#2},},}
                newcommand{totald}[3]{frac{mathrm{d}^{#1} #2}{mathrm{d} #3^{#1}}}
                newcommand{verts}[1]{leftvert,{#1},rightvert}$
                begin{align}
                &lim_{n to infty}braces{int_{0}^{1}bracks{bx + apars{1 - x}}^{1/n}
                ,dd x}^{n} =
                lim_{n to infty}bracks{{1 over b - a}int_{a}^{b}x^{1/n}
                ,dd x}^{n}
                \[5mm] &=
                lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} + lnpars{int_{a}^{b}x^{epsilon},dd x} over epsilon}
                \[5mm] & =
                lim_{epsilon to 0^{+}}exppars{-lnpars{b - a} +
                lnpars{b^{epsilon + 1} - a^{epsilon + 1}} - lnpars{epsilon + 1} over epsilon}
                \[5mm] & =
                lim_{epsilon to 0^{+}}exppars{
                {b^{epsilon + 1}lnpars{b} - a^{epsilon + 1}lnpars{a} over b^{epsilon + 1} - a^{epsilon + 1}} - {1 over epsilon + 1}}qquadqquad
                pars{~L'Hhat{o}pital Rule~}
                \[5mm] & =
                exppars{{blnpars{b} - alnpars{a} over b - a} - 1} =
                bbx{ds{{1 over expo{}},pars{b^{b} over a^{a}}^{1/pars{b - a}}}}
                end{align}







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Oct 19 '16 at 22:58









                Felix Marin

                67.1k7107141




                67.1k7107141






























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