Convergence of $int_0^{frac{pi}{2}} frac{exp({-1/x)}}{sqrt{ sin x}}, mathrm{d}x$












1












$begingroup$


Let $$f(x)=frac{exp(-1/x)}{sqrt{ sin x}}, mathrm{d}x.$$



$f(x)$ seems to not have any problems at $x=frac {pi}{2}$, but at $x=0$.

So I should understand behavior of $f(x)$ at $x=0$ by evaluating $lim_{xto0+}f(x)$.But I am stuck here as I can't apply Taylor expansions to $e^{-frac{1}{x}}$ and using l'Hospital's rule gives me nothing.










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$endgroup$








  • 1




    $begingroup$
    You could try squaring $f$ first, then compute the limit at $0$.
    $endgroup$
    – user170231
    Jan 12 at 21:25










  • $begingroup$
    @user170231 what exactly lets us squaring $f$ and then take the limit?
    $endgroup$
    – Turan Nəsibli
    Jan 12 at 21:31
















1












$begingroup$


Let $$f(x)=frac{exp(-1/x)}{sqrt{ sin x}}, mathrm{d}x.$$



$f(x)$ seems to not have any problems at $x=frac {pi}{2}$, but at $x=0$.

So I should understand behavior of $f(x)$ at $x=0$ by evaluating $lim_{xto0+}f(x)$.But I am stuck here as I can't apply Taylor expansions to $e^{-frac{1}{x}}$ and using l'Hospital's rule gives me nothing.










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    You could try squaring $f$ first, then compute the limit at $0$.
    $endgroup$
    – user170231
    Jan 12 at 21:25










  • $begingroup$
    @user170231 what exactly lets us squaring $f$ and then take the limit?
    $endgroup$
    – Turan Nəsibli
    Jan 12 at 21:31














1












1








1





$begingroup$


Let $$f(x)=frac{exp(-1/x)}{sqrt{ sin x}}, mathrm{d}x.$$



$f(x)$ seems to not have any problems at $x=frac {pi}{2}$, but at $x=0$.

So I should understand behavior of $f(x)$ at $x=0$ by evaluating $lim_{xto0+}f(x)$.But I am stuck here as I can't apply Taylor expansions to $e^{-frac{1}{x}}$ and using l'Hospital's rule gives me nothing.










share|cite|improve this question











$endgroup$




Let $$f(x)=frac{exp(-1/x)}{sqrt{ sin x}}, mathrm{d}x.$$



$f(x)$ seems to not have any problems at $x=frac {pi}{2}$, but at $x=0$.

So I should understand behavior of $f(x)$ at $x=0$ by evaluating $lim_{xto0+}f(x)$.But I am stuck here as I can't apply Taylor expansions to $e^{-frac{1}{x}}$ and using l'Hospital's rule gives me nothing.







calculus limits improper-integrals






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edited Jan 12 at 21:17









Clayton

19.1k33285




19.1k33285










asked Jan 12 at 21:14









Turan NəsibliTuran Nəsibli

776




776








  • 1




    $begingroup$
    You could try squaring $f$ first, then compute the limit at $0$.
    $endgroup$
    – user170231
    Jan 12 at 21:25










  • $begingroup$
    @user170231 what exactly lets us squaring $f$ and then take the limit?
    $endgroup$
    – Turan Nəsibli
    Jan 12 at 21:31














  • 1




    $begingroup$
    You could try squaring $f$ first, then compute the limit at $0$.
    $endgroup$
    – user170231
    Jan 12 at 21:25










  • $begingroup$
    @user170231 what exactly lets us squaring $f$ and then take the limit?
    $endgroup$
    – Turan Nəsibli
    Jan 12 at 21:31








1




1




$begingroup$
You could try squaring $f$ first, then compute the limit at $0$.
$endgroup$
– user170231
Jan 12 at 21:25




$begingroup$
You could try squaring $f$ first, then compute the limit at $0$.
$endgroup$
– user170231
Jan 12 at 21:25












$begingroup$
@user170231 what exactly lets us squaring $f$ and then take the limit?
$endgroup$
– Turan Nəsibli
Jan 12 at 21:31




$begingroup$
@user170231 what exactly lets us squaring $f$ and then take the limit?
$endgroup$
– Turan Nəsibli
Jan 12 at 21:31










2 Answers
2






active

oldest

votes


















3












$begingroup$

Note that $e^{1/x}ge 1+frac1x$ for $x>0$ and $xcos(x)le sin(x)$ for $xin [0,pi/2]$.



Hence for $xin(0,pi/2]$, we have



$$0le frac{e^{-1/x}}{sqrt{sin(x)}}le frac{1}{left(1+frac 1xright) sqrt{xcos(x)}}=frac{sqrt x}{x+1}sqrt{frac{
1}{cos(x)}} $$



Now apply the squeeze theorem.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Can you please explain your comment on my answer, since your comment is not constructive?
    $endgroup$
    – Viktor Glombik
    Jan 13 at 20:53










  • $begingroup$
    @viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:13










  • $begingroup$
    You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:37












  • $begingroup$
    I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
    $endgroup$
    – Viktor Glombik
    Jan 14 at 0:57












  • $begingroup$
    Viktor I don't have time to rewrite your post.
    $endgroup$
    – Mark Viola
    Jan 14 at 1:24



















2












$begingroup$

Using the continuity of the square root, we can conclude
begin{equation*}
I
:=lim_{x searrow 0} frac{e^{-frac{1}{x}}}{sqrt{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{e^{-frac{2}{x}}}{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{1}{e^{frac{2}{x}} sin(x)}}
end{equation*}

Now, we can apply L'Hôpital to the following limit
begin{equation*}
L
:= lim_{x searrow 0} e^{frac{2}{x}} sin(x)
= lim_{x searrow 0} frac{x^2}{2} cos(x) cdot e^{frac{2}{x}}
end{equation*}

And now, because the limits of the factors exist and are finite
begin{equation*}
L = frac{1}{2} underbrace{lim_{x searrow 0} cos(x)}_{= 1} cdot left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)
= frac{1}{2} underbrace{left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)}_{:= widetilde{L}}
end{equation*}



Since $x mapsto x^2$ is monotone and continuous, we have
begin{equation*}
widetilde{L}
= big( underbrace{lim_{x searrow 0} x cdot e^{frac{1}{x}}}_{=: widehat{L}} big)^2
end{equation*}

Now, by L'Hôpital, we have
begin{equation*}
widehat{L}
= lim_{x searrow 0} frac{e^{frac{1}{x}}}{frac{1}{x}}
= lim_{x searrow 0} frac{frac{d}{dx} e^{frac{1}{x}}}{frac{d}{dx} frac{1}{x}}
= lim_{x searrow 0} frac{-frac{1}{x^2} e^{frac{1}{x}}}{-frac{1}{x^2}}
= lim_{x searrow 0} e^{frac{1}{x}}
= infty.
end{equation*}



Therefore, we have $L = infty$ and so $I = 0$.






share|cite|improve this answer











$endgroup$









  • 2




    $begingroup$
    This makes no sense.
    $endgroup$
    – Mark Viola
    Jan 12 at 22:09











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2 Answers
2






active

oldest

votes








2 Answers
2






active

oldest

votes









active

oldest

votes






active

oldest

votes









3












$begingroup$

Note that $e^{1/x}ge 1+frac1x$ for $x>0$ and $xcos(x)le sin(x)$ for $xin [0,pi/2]$.



Hence for $xin(0,pi/2]$, we have



$$0le frac{e^{-1/x}}{sqrt{sin(x)}}le frac{1}{left(1+frac 1xright) sqrt{xcos(x)}}=frac{sqrt x}{x+1}sqrt{frac{
1}{cos(x)}} $$



Now apply the squeeze theorem.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Can you please explain your comment on my answer, since your comment is not constructive?
    $endgroup$
    – Viktor Glombik
    Jan 13 at 20:53










  • $begingroup$
    @viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:13










  • $begingroup$
    You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:37












  • $begingroup$
    I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
    $endgroup$
    – Viktor Glombik
    Jan 14 at 0:57












  • $begingroup$
    Viktor I don't have time to rewrite your post.
    $endgroup$
    – Mark Viola
    Jan 14 at 1:24
















3












$begingroup$

Note that $e^{1/x}ge 1+frac1x$ for $x>0$ and $xcos(x)le sin(x)$ for $xin [0,pi/2]$.



Hence for $xin(0,pi/2]$, we have



$$0le frac{e^{-1/x}}{sqrt{sin(x)}}le frac{1}{left(1+frac 1xright) sqrt{xcos(x)}}=frac{sqrt x}{x+1}sqrt{frac{
1}{cos(x)}} $$



Now apply the squeeze theorem.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Can you please explain your comment on my answer, since your comment is not constructive?
    $endgroup$
    – Viktor Glombik
    Jan 13 at 20:53










  • $begingroup$
    @viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:13










  • $begingroup$
    You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:37












  • $begingroup$
    I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
    $endgroup$
    – Viktor Glombik
    Jan 14 at 0:57












  • $begingroup$
    Viktor I don't have time to rewrite your post.
    $endgroup$
    – Mark Viola
    Jan 14 at 1:24














3












3








3





$begingroup$

Note that $e^{1/x}ge 1+frac1x$ for $x>0$ and $xcos(x)le sin(x)$ for $xin [0,pi/2]$.



Hence for $xin(0,pi/2]$, we have



$$0le frac{e^{-1/x}}{sqrt{sin(x)}}le frac{1}{left(1+frac 1xright) sqrt{xcos(x)}}=frac{sqrt x}{x+1}sqrt{frac{
1}{cos(x)}} $$



Now apply the squeeze theorem.






share|cite|improve this answer











$endgroup$



Note that $e^{1/x}ge 1+frac1x$ for $x>0$ and $xcos(x)le sin(x)$ for $xin [0,pi/2]$.



Hence for $xin(0,pi/2]$, we have



$$0le frac{e^{-1/x}}{sqrt{sin(x)}}le frac{1}{left(1+frac 1xright) sqrt{xcos(x)}}=frac{sqrt x}{x+1}sqrt{frac{
1}{cos(x)}} $$



Now apply the squeeze theorem.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Jan 13 at 19:16

























answered Jan 12 at 22:14









Mark ViolaMark Viola

132k1275173




132k1275173












  • $begingroup$
    Can you please explain your comment on my answer, since your comment is not constructive?
    $endgroup$
    – Viktor Glombik
    Jan 13 at 20:53










  • $begingroup$
    @viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:13










  • $begingroup$
    You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:37












  • $begingroup$
    I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
    $endgroup$
    – Viktor Glombik
    Jan 14 at 0:57












  • $begingroup$
    Viktor I don't have time to rewrite your post.
    $endgroup$
    – Mark Viola
    Jan 14 at 1:24


















  • $begingroup$
    Can you please explain your comment on my answer, since your comment is not constructive?
    $endgroup$
    – Viktor Glombik
    Jan 13 at 20:53










  • $begingroup$
    @viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:13










  • $begingroup$
    You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
    $endgroup$
    – Mark Viola
    Jan 13 at 23:37












  • $begingroup$
    I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
    $endgroup$
    – Viktor Glombik
    Jan 14 at 0:57












  • $begingroup$
    Viktor I don't have time to rewrite your post.
    $endgroup$
    – Mark Viola
    Jan 14 at 1:24
















$begingroup$
Can you please explain your comment on my answer, since your comment is not constructive?
$endgroup$
– Viktor Glombik
Jan 13 at 20:53




$begingroup$
Can you please explain your comment on my answer, since your comment is not constructive?
$endgroup$
– Viktor Glombik
Jan 13 at 20:53












$begingroup$
@viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
$endgroup$
– Mark Viola
Jan 13 at 23:13




$begingroup$
@viktorglombik For example, your use of LHR after you wrote "Now we can apply ..." makes no sense whatsoever.
$endgroup$
– Mark Viola
Jan 13 at 23:13












$begingroup$
You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
$endgroup$
– Mark Viola
Jan 13 at 23:37






$begingroup$
You can apply LHR if the limit of the quotient of derivatives exists. Have you shown this here? The limit does exist and is $0$, but you haven't shown this. At best your development is convoluted. And writing $L=2(infty)^2$ is definitely nonsense.
$endgroup$
– Mark Viola
Jan 13 at 23:37














$begingroup$
I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
$endgroup$
– Viktor Glombik
Jan 14 at 0:57






$begingroup$
I have shown $f(x) to infty$, so $frac{1}{f(x)} to 0$ follows, when minding the appropriate restrictions. If you have a good idea on improving my answer, please edit it! We're all here to learn, after all.
$endgroup$
– Viktor Glombik
Jan 14 at 0:57














$begingroup$
Viktor I don't have time to rewrite your post.
$endgroup$
– Mark Viola
Jan 14 at 1:24




$begingroup$
Viktor I don't have time to rewrite your post.
$endgroup$
– Mark Viola
Jan 14 at 1:24











2












$begingroup$

Using the continuity of the square root, we can conclude
begin{equation*}
I
:=lim_{x searrow 0} frac{e^{-frac{1}{x}}}{sqrt{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{e^{-frac{2}{x}}}{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{1}{e^{frac{2}{x}} sin(x)}}
end{equation*}

Now, we can apply L'Hôpital to the following limit
begin{equation*}
L
:= lim_{x searrow 0} e^{frac{2}{x}} sin(x)
= lim_{x searrow 0} frac{x^2}{2} cos(x) cdot e^{frac{2}{x}}
end{equation*}

And now, because the limits of the factors exist and are finite
begin{equation*}
L = frac{1}{2} underbrace{lim_{x searrow 0} cos(x)}_{= 1} cdot left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)
= frac{1}{2} underbrace{left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)}_{:= widetilde{L}}
end{equation*}



Since $x mapsto x^2$ is monotone and continuous, we have
begin{equation*}
widetilde{L}
= big( underbrace{lim_{x searrow 0} x cdot e^{frac{1}{x}}}_{=: widehat{L}} big)^2
end{equation*}

Now, by L'Hôpital, we have
begin{equation*}
widehat{L}
= lim_{x searrow 0} frac{e^{frac{1}{x}}}{frac{1}{x}}
= lim_{x searrow 0} frac{frac{d}{dx} e^{frac{1}{x}}}{frac{d}{dx} frac{1}{x}}
= lim_{x searrow 0} frac{-frac{1}{x^2} e^{frac{1}{x}}}{-frac{1}{x^2}}
= lim_{x searrow 0} e^{frac{1}{x}}
= infty.
end{equation*}



Therefore, we have $L = infty$ and so $I = 0$.






share|cite|improve this answer











$endgroup$









  • 2




    $begingroup$
    This makes no sense.
    $endgroup$
    – Mark Viola
    Jan 12 at 22:09
















2












$begingroup$

Using the continuity of the square root, we can conclude
begin{equation*}
I
:=lim_{x searrow 0} frac{e^{-frac{1}{x}}}{sqrt{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{e^{-frac{2}{x}}}{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{1}{e^{frac{2}{x}} sin(x)}}
end{equation*}

Now, we can apply L'Hôpital to the following limit
begin{equation*}
L
:= lim_{x searrow 0} e^{frac{2}{x}} sin(x)
= lim_{x searrow 0} frac{x^2}{2} cos(x) cdot e^{frac{2}{x}}
end{equation*}

And now, because the limits of the factors exist and are finite
begin{equation*}
L = frac{1}{2} underbrace{lim_{x searrow 0} cos(x)}_{= 1} cdot left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)
= frac{1}{2} underbrace{left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)}_{:= widetilde{L}}
end{equation*}



Since $x mapsto x^2$ is monotone and continuous, we have
begin{equation*}
widetilde{L}
= big( underbrace{lim_{x searrow 0} x cdot e^{frac{1}{x}}}_{=: widehat{L}} big)^2
end{equation*}

Now, by L'Hôpital, we have
begin{equation*}
widehat{L}
= lim_{x searrow 0} frac{e^{frac{1}{x}}}{frac{1}{x}}
= lim_{x searrow 0} frac{frac{d}{dx} e^{frac{1}{x}}}{frac{d}{dx} frac{1}{x}}
= lim_{x searrow 0} frac{-frac{1}{x^2} e^{frac{1}{x}}}{-frac{1}{x^2}}
= lim_{x searrow 0} e^{frac{1}{x}}
= infty.
end{equation*}



Therefore, we have $L = infty$ and so $I = 0$.






share|cite|improve this answer











$endgroup$









  • 2




    $begingroup$
    This makes no sense.
    $endgroup$
    – Mark Viola
    Jan 12 at 22:09














2












2








2





$begingroup$

Using the continuity of the square root, we can conclude
begin{equation*}
I
:=lim_{x searrow 0} frac{e^{-frac{1}{x}}}{sqrt{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{e^{-frac{2}{x}}}{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{1}{e^{frac{2}{x}} sin(x)}}
end{equation*}

Now, we can apply L'Hôpital to the following limit
begin{equation*}
L
:= lim_{x searrow 0} e^{frac{2}{x}} sin(x)
= lim_{x searrow 0} frac{x^2}{2} cos(x) cdot e^{frac{2}{x}}
end{equation*}

And now, because the limits of the factors exist and are finite
begin{equation*}
L = frac{1}{2} underbrace{lim_{x searrow 0} cos(x)}_{= 1} cdot left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)
= frac{1}{2} underbrace{left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)}_{:= widetilde{L}}
end{equation*}



Since $x mapsto x^2$ is monotone and continuous, we have
begin{equation*}
widetilde{L}
= big( underbrace{lim_{x searrow 0} x cdot e^{frac{1}{x}}}_{=: widehat{L}} big)^2
end{equation*}

Now, by L'Hôpital, we have
begin{equation*}
widehat{L}
= lim_{x searrow 0} frac{e^{frac{1}{x}}}{frac{1}{x}}
= lim_{x searrow 0} frac{frac{d}{dx} e^{frac{1}{x}}}{frac{d}{dx} frac{1}{x}}
= lim_{x searrow 0} frac{-frac{1}{x^2} e^{frac{1}{x}}}{-frac{1}{x^2}}
= lim_{x searrow 0} e^{frac{1}{x}}
= infty.
end{equation*}



Therefore, we have $L = infty$ and so $I = 0$.






share|cite|improve this answer











$endgroup$



Using the continuity of the square root, we can conclude
begin{equation*}
I
:=lim_{x searrow 0} frac{e^{-frac{1}{x}}}{sqrt{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{e^{-frac{2}{x}}}{sin(x)}}
= sqrt{ lim_{x searrow 0} frac{1}{e^{frac{2}{x}} sin(x)}}
end{equation*}

Now, we can apply L'Hôpital to the following limit
begin{equation*}
L
:= lim_{x searrow 0} e^{frac{2}{x}} sin(x)
= lim_{x searrow 0} frac{x^2}{2} cos(x) cdot e^{frac{2}{x}}
end{equation*}

And now, because the limits of the factors exist and are finite
begin{equation*}
L = frac{1}{2} underbrace{lim_{x searrow 0} cos(x)}_{= 1} cdot left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)
= frac{1}{2} underbrace{left(lim_{x searrow 0} x^2 cdot e^{frac{2}{x}}right)}_{:= widetilde{L}}
end{equation*}



Since $x mapsto x^2$ is monotone and continuous, we have
begin{equation*}
widetilde{L}
= big( underbrace{lim_{x searrow 0} x cdot e^{frac{1}{x}}}_{=: widehat{L}} big)^2
end{equation*}

Now, by L'Hôpital, we have
begin{equation*}
widehat{L}
= lim_{x searrow 0} frac{e^{frac{1}{x}}}{frac{1}{x}}
= lim_{x searrow 0} frac{frac{d}{dx} e^{frac{1}{x}}}{frac{d}{dx} frac{1}{x}}
= lim_{x searrow 0} frac{-frac{1}{x^2} e^{frac{1}{x}}}{-frac{1}{x^2}}
= lim_{x searrow 0} e^{frac{1}{x}}
= infty.
end{equation*}



Therefore, we have $L = infty$ and so $I = 0$.







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edited Jan 14 at 0:56

























answered Jan 12 at 21:57









Viktor GlombikViktor Glombik

9251527




9251527








  • 2




    $begingroup$
    This makes no sense.
    $endgroup$
    – Mark Viola
    Jan 12 at 22:09














  • 2




    $begingroup$
    This makes no sense.
    $endgroup$
    – Mark Viola
    Jan 12 at 22:09








2




2




$begingroup$
This makes no sense.
$endgroup$
– Mark Viola
Jan 12 at 22:09




$begingroup$
This makes no sense.
$endgroup$
– Mark Viola
Jan 12 at 22:09


















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