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How to prove this integral is convergent [on hold]


Integral in d-dimensionsHow prove this integral $int_0^inftyf^alpha(x)dx,alpha>1$ is convergentHow do you find the limits of integration without drawing a picture?How to calculate the integral of a function defined by polar variables?Why is this integral not absolutely integrable?Does this double integral converge?Showing that $int_0^infty cfrac1x^2+tdx$ is convergent for $t>0$polar coordinates for integral bounds with parallelogram as regionHow I can evaluate this integral?Prove that this integral with exponent with whole part is convergent













0












$begingroup$


I have to prove that this integral is convergent:



$ int_vertxivert geq 1 vertxivert^-2[fracn2]-2 dxi $



where $ n $ is the dimension of $ R^n $ and $ [ cdot] $ denotes the floor function. Maybe polar coordinates can be used, but i don't know how to prove that is convergent. Can anyone help me?



Thank you.










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put on hold as off-topic by uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa 2 days ago


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa
If this question can be reworded to fit the rules in the help center, please edit the question.















  • $begingroup$
    Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
    $endgroup$
    – uniquesolution
    Mar 11 at 8:40















0












$begingroup$


I have to prove that this integral is convergent:



$ int_vertxivert geq 1 vertxivert^-2[fracn2]-2 dxi $



where $ n $ is the dimension of $ R^n $ and $ [ cdot] $ denotes the floor function. Maybe polar coordinates can be used, but i don't know how to prove that is convergent. Can anyone help me?



Thank you.










share|cite|improve this question









$endgroup$



put on hold as off-topic by uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa 2 days ago


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa
If this question can be reworded to fit the rules in the help center, please edit the question.















  • $begingroup$
    Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
    $endgroup$
    – uniquesolution
    Mar 11 at 8:40













0












0








0





$begingroup$


I have to prove that this integral is convergent:



$ int_vertxivert geq 1 vertxivert^-2[fracn2]-2 dxi $



where $ n $ is the dimension of $ R^n $ and $ [ cdot] $ denotes the floor function. Maybe polar coordinates can be used, but i don't know how to prove that is convergent. Can anyone help me?



Thank you.










share|cite|improve this question









$endgroup$




I have to prove that this integral is convergent:



$ int_vertxivert geq 1 vertxivert^-2[fracn2]-2 dxi $



where $ n $ is the dimension of $ R^n $ and $ [ cdot] $ denotes the floor function. Maybe polar coordinates can be used, but i don't know how to prove that is convergent. Can anyone help me?



Thank you.







real-analysis integration convergence polar-coordinates






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share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Mar 11 at 8:36









C. BishopC. Bishop

84




84




put on hold as off-topic by uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa 2 days ago


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa
If this question can be reworded to fit the rules in the help center, please edit the question.







put on hold as off-topic by uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa 2 days ago


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – uniquesolution, José Carlos Santos, GNUSupporter 8964民主女神 地下教會, Leucippus, Vinyl_cape_jawa
If this question can be reworded to fit the rules in the help center, please edit the question.











  • $begingroup$
    Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
    $endgroup$
    – uniquesolution
    Mar 11 at 8:40
















  • $begingroup$
    Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
    $endgroup$
    – uniquesolution
    Mar 11 at 8:40















$begingroup$
Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
$endgroup$
– uniquesolution
Mar 11 at 8:40




$begingroup$
Yes, maybe polar coordinates can be used. Why don't you try and tell us what you got?
$endgroup$
– uniquesolution
Mar 11 at 8:40










2 Answers
2






active

oldest

votes


















0












$begingroup$

In order to define polar coordinates in $n$ dimensions, we need $n+1$ angular variables. One way to set this up is to take a hint from three-dimensional spherical coordinates; define $x_1=rcostheta_1$, $x_2=rsintheta_1costheta_2$, $x_3=rsintheta_1sintheta_2costheta_3$, and so on until we close it with $x_n=rsintheta_1sintheta_2sintheta_3cdots sintheta_n-1$. In transforming to these coordinates, the Jacobian will be something involving the angular variables times $r^n-1$. If we integrate a radially symmetric function $f(|x|)$ over the radially symmetric region $|x|>1$, we get a constant from the $theta$ integrals and
$$int_xf(x),dx_1,dx_2,cdots,dx_n = A(n)int_1^inftyr^n-1f(r),dr$$
where $A(n)$ depends only on $n$. For $f(r)=r^-2lfloor n/2rfloor-2$, that leads us to the integral of $r^-3$ or $r^-2$, depending on whether $n$ is even or odd. You should know how to handle the convergence of a one-dimensional integral like this.



We can also avoid having to define these coordinates. It is well-known that every norm on $mathbbR^n$ is equivalent - so let's work with a more convenient norm. The $infty$-norm $|x|_infty=maxx_1,x_2,dots,x_n$ is particularly easy to work with for integrals, as it will naturally depend (locally) on only one of the variables. In converting between norms, we have that $|x|_2le sqrtn|x|_infty$ and $|x|_infty le |x|_2$.



So then, increasing first the region and then the integrand,
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_infty^-2lfloor n/2rfloor-2,dx=I$$
Now, we integrate that. Split the region based on which coordinate is largest and whether it's positive or negative; we get $2n$ regions this way, of which the first is $x_1ge |x_2|,|x_3|,dots,|x_n|$. By symmetry, the integral over each of these regions is equal, and
$$I = 2nint_1/sqrtn^inftyint_-x_1^x_1cdots int_-x_1^x_1x_1^-2lfloor n/2rfloor-2,dx_n,cdots,dx_2,dx_1 = 2nint_1/sqrtn^infty2^n-1x_1^n-2lfloor n/2rfloor-3,dx_1$$
Then $n-2lfloor n/2rfloor=begincases0&ntext is even\1&ntext is oddendcases$. For even $n$, we get
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-3,dx=left. -2^n-1 nx_1^-2right|_1/sqrtn^infty=2^n-1$$
For odd $n$, we instead have
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-2,dx=left. -2^n nx_1^-1right|_1/sqrtn^infty=2^nsqrtn$$
Either way, the original integral converges by comparison.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    You've been really really clear. Thank you so much!
    $endgroup$
    – C. Bishop
    Mar 11 at 10:09


















0












$begingroup$

Just you polar coordinates and consider the cases $n$ even and $n$ odd separately. The integral is convergent in both cases.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
    $endgroup$
    – C. Bishop
    Mar 11 at 8:48










  • $begingroup$
    If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
    $endgroup$
    – Kavi Rama Murthy
    Mar 11 at 8:49

















2 Answers
2






active

oldest

votes








2 Answers
2






active

oldest

votes









active

oldest

votes






active

oldest

votes









0












$begingroup$

In order to define polar coordinates in $n$ dimensions, we need $n+1$ angular variables. One way to set this up is to take a hint from three-dimensional spherical coordinates; define $x_1=rcostheta_1$, $x_2=rsintheta_1costheta_2$, $x_3=rsintheta_1sintheta_2costheta_3$, and so on until we close it with $x_n=rsintheta_1sintheta_2sintheta_3cdots sintheta_n-1$. In transforming to these coordinates, the Jacobian will be something involving the angular variables times $r^n-1$. If we integrate a radially symmetric function $f(|x|)$ over the radially symmetric region $|x|>1$, we get a constant from the $theta$ integrals and
$$int_xf(x),dx_1,dx_2,cdots,dx_n = A(n)int_1^inftyr^n-1f(r),dr$$
where $A(n)$ depends only on $n$. For $f(r)=r^-2lfloor n/2rfloor-2$, that leads us to the integral of $r^-3$ or $r^-2$, depending on whether $n$ is even or odd. You should know how to handle the convergence of a one-dimensional integral like this.



We can also avoid having to define these coordinates. It is well-known that every norm on $mathbbR^n$ is equivalent - so let's work with a more convenient norm. The $infty$-norm $|x|_infty=maxx_1,x_2,dots,x_n$ is particularly easy to work with for integrals, as it will naturally depend (locally) on only one of the variables. In converting between norms, we have that $|x|_2le sqrtn|x|_infty$ and $|x|_infty le |x|_2$.



So then, increasing first the region and then the integrand,
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_infty^-2lfloor n/2rfloor-2,dx=I$$
Now, we integrate that. Split the region based on which coordinate is largest and whether it's positive or negative; we get $2n$ regions this way, of which the first is $x_1ge |x_2|,|x_3|,dots,|x_n|$. By symmetry, the integral over each of these regions is equal, and
$$I = 2nint_1/sqrtn^inftyint_-x_1^x_1cdots int_-x_1^x_1x_1^-2lfloor n/2rfloor-2,dx_n,cdots,dx_2,dx_1 = 2nint_1/sqrtn^infty2^n-1x_1^n-2lfloor n/2rfloor-3,dx_1$$
Then $n-2lfloor n/2rfloor=begincases0&ntext is even\1&ntext is oddendcases$. For even $n$, we get
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-3,dx=left. -2^n-1 nx_1^-2right|_1/sqrtn^infty=2^n-1$$
For odd $n$, we instead have
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-2,dx=left. -2^n nx_1^-1right|_1/sqrtn^infty=2^nsqrtn$$
Either way, the original integral converges by comparison.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    You've been really really clear. Thank you so much!
    $endgroup$
    – C. Bishop
    Mar 11 at 10:09















0












$begingroup$

In order to define polar coordinates in $n$ dimensions, we need $n+1$ angular variables. One way to set this up is to take a hint from three-dimensional spherical coordinates; define $x_1=rcostheta_1$, $x_2=rsintheta_1costheta_2$, $x_3=rsintheta_1sintheta_2costheta_3$, and so on until we close it with $x_n=rsintheta_1sintheta_2sintheta_3cdots sintheta_n-1$. In transforming to these coordinates, the Jacobian will be something involving the angular variables times $r^n-1$. If we integrate a radially symmetric function $f(|x|)$ over the radially symmetric region $|x|>1$, we get a constant from the $theta$ integrals and
$$int_xf(x),dx_1,dx_2,cdots,dx_n = A(n)int_1^inftyr^n-1f(r),dr$$
where $A(n)$ depends only on $n$. For $f(r)=r^-2lfloor n/2rfloor-2$, that leads us to the integral of $r^-3$ or $r^-2$, depending on whether $n$ is even or odd. You should know how to handle the convergence of a one-dimensional integral like this.



We can also avoid having to define these coordinates. It is well-known that every norm on $mathbbR^n$ is equivalent - so let's work with a more convenient norm. The $infty$-norm $|x|_infty=maxx_1,x_2,dots,x_n$ is particularly easy to work with for integrals, as it will naturally depend (locally) on only one of the variables. In converting between norms, we have that $|x|_2le sqrtn|x|_infty$ and $|x|_infty le |x|_2$.



So then, increasing first the region and then the integrand,
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_infty^-2lfloor n/2rfloor-2,dx=I$$
Now, we integrate that. Split the region based on which coordinate is largest and whether it's positive or negative; we get $2n$ regions this way, of which the first is $x_1ge |x_2|,|x_3|,dots,|x_n|$. By symmetry, the integral over each of these regions is equal, and
$$I = 2nint_1/sqrtn^inftyint_-x_1^x_1cdots int_-x_1^x_1x_1^-2lfloor n/2rfloor-2,dx_n,cdots,dx_2,dx_1 = 2nint_1/sqrtn^infty2^n-1x_1^n-2lfloor n/2rfloor-3,dx_1$$
Then $n-2lfloor n/2rfloor=begincases0&ntext is even\1&ntext is oddendcases$. For even $n$, we get
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-3,dx=left. -2^n-1 nx_1^-2right|_1/sqrtn^infty=2^n-1$$
For odd $n$, we instead have
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-2,dx=left. -2^n nx_1^-1right|_1/sqrtn^infty=2^nsqrtn$$
Either way, the original integral converges by comparison.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    You've been really really clear. Thank you so much!
    $endgroup$
    – C. Bishop
    Mar 11 at 10:09













0












0








0





$begingroup$

In order to define polar coordinates in $n$ dimensions, we need $n+1$ angular variables. One way to set this up is to take a hint from three-dimensional spherical coordinates; define $x_1=rcostheta_1$, $x_2=rsintheta_1costheta_2$, $x_3=rsintheta_1sintheta_2costheta_3$, and so on until we close it with $x_n=rsintheta_1sintheta_2sintheta_3cdots sintheta_n-1$. In transforming to these coordinates, the Jacobian will be something involving the angular variables times $r^n-1$. If we integrate a radially symmetric function $f(|x|)$ over the radially symmetric region $|x|>1$, we get a constant from the $theta$ integrals and
$$int_xf(x),dx_1,dx_2,cdots,dx_n = A(n)int_1^inftyr^n-1f(r),dr$$
where $A(n)$ depends only on $n$. For $f(r)=r^-2lfloor n/2rfloor-2$, that leads us to the integral of $r^-3$ or $r^-2$, depending on whether $n$ is even or odd. You should know how to handle the convergence of a one-dimensional integral like this.



We can also avoid having to define these coordinates. It is well-known that every norm on $mathbbR^n$ is equivalent - so let's work with a more convenient norm. The $infty$-norm $|x|_infty=maxx_1,x_2,dots,x_n$ is particularly easy to work with for integrals, as it will naturally depend (locally) on only one of the variables. In converting between norms, we have that $|x|_2le sqrtn|x|_infty$ and $|x|_infty le |x|_2$.



So then, increasing first the region and then the integrand,
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_infty^-2lfloor n/2rfloor-2,dx=I$$
Now, we integrate that. Split the region based on which coordinate is largest and whether it's positive or negative; we get $2n$ regions this way, of which the first is $x_1ge |x_2|,|x_3|,dots,|x_n|$. By symmetry, the integral over each of these regions is equal, and
$$I = 2nint_1/sqrtn^inftyint_-x_1^x_1cdots int_-x_1^x_1x_1^-2lfloor n/2rfloor-2,dx_n,cdots,dx_2,dx_1 = 2nint_1/sqrtn^infty2^n-1x_1^n-2lfloor n/2rfloor-3,dx_1$$
Then $n-2lfloor n/2rfloor=begincases0&ntext is even\1&ntext is oddendcases$. For even $n$, we get
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-3,dx=left. -2^n-1 nx_1^-2right|_1/sqrtn^infty=2^n-1$$
For odd $n$, we instead have
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-2,dx=left. -2^n nx_1^-1right|_1/sqrtn^infty=2^nsqrtn$$
Either way, the original integral converges by comparison.






share|cite|improve this answer











$endgroup$



In order to define polar coordinates in $n$ dimensions, we need $n+1$ angular variables. One way to set this up is to take a hint from three-dimensional spherical coordinates; define $x_1=rcostheta_1$, $x_2=rsintheta_1costheta_2$, $x_3=rsintheta_1sintheta_2costheta_3$, and so on until we close it with $x_n=rsintheta_1sintheta_2sintheta_3cdots sintheta_n-1$. In transforming to these coordinates, the Jacobian will be something involving the angular variables times $r^n-1$. If we integrate a radially symmetric function $f(|x|)$ over the radially symmetric region $|x|>1$, we get a constant from the $theta$ integrals and
$$int_xf(x),dx_1,dx_2,cdots,dx_n = A(n)int_1^inftyr^n-1f(r),dr$$
where $A(n)$ depends only on $n$. For $f(r)=r^-2lfloor n/2rfloor-2$, that leads us to the integral of $r^-3$ or $r^-2$, depending on whether $n$ is even or odd. You should know how to handle the convergence of a one-dimensional integral like this.



We can also avoid having to define these coordinates. It is well-known that every norm on $mathbbR^n$ is equivalent - so let's work with a more convenient norm. The $infty$-norm $|x|_infty=maxx_1,x_2,dots,x_n$ is particularly easy to work with for integrals, as it will naturally depend (locally) on only one of the variables. In converting between norms, we have that $|x|_2le sqrtn|x|_infty$ and $|x|_infty le |x|_2$.



So then, increasing first the region and then the integrand,
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_2^-2lfloor n/2rfloor-2,dx le int_|x|_infty^-2lfloor n/2rfloor-2,dx=I$$
Now, we integrate that. Split the region based on which coordinate is largest and whether it's positive or negative; we get $2n$ regions this way, of which the first is $x_1ge |x_2|,|x_3|,dots,|x_n|$. By symmetry, the integral over each of these regions is equal, and
$$I = 2nint_1/sqrtn^inftyint_-x_1^x_1cdots int_-x_1^x_1x_1^-2lfloor n/2rfloor-2,dx_n,cdots,dx_2,dx_1 = 2nint_1/sqrtn^infty2^n-1x_1^n-2lfloor n/2rfloor-3,dx_1$$
Then $n-2lfloor n/2rfloor=begincases0&ntext is even\1&ntext is oddendcases$. For even $n$, we get
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-3,dx=left. -2^n-1 nx_1^-2right|_1/sqrtn^infty=2^n-1$$
For odd $n$, we instead have
$$int_x|x|_2^-2lfloor n/2rfloor-2,dx le I=2^n nint_1/sqrtn^inftyx_1^-2,dx=left. -2^n nx_1^-1right|_1/sqrtn^infty=2^nsqrtn$$
Either way, the original integral converges by comparison.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Mar 11 at 9:29

























answered Mar 11 at 9:22









jmerryjmerry

14k1629




14k1629











  • $begingroup$
    You've been really really clear. Thank you so much!
    $endgroup$
    – C. Bishop
    Mar 11 at 10:09
















  • $begingroup$
    You've been really really clear. Thank you so much!
    $endgroup$
    – C. Bishop
    Mar 11 at 10:09















$begingroup$
You've been really really clear. Thank you so much!
$endgroup$
– C. Bishop
Mar 11 at 10:09




$begingroup$
You've been really really clear. Thank you so much!
$endgroup$
– C. Bishop
Mar 11 at 10:09











0












$begingroup$

Just you polar coordinates and consider the cases $n$ even and $n$ odd separately. The integral is convergent in both cases.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
    $endgroup$
    – C. Bishop
    Mar 11 at 8:48










  • $begingroup$
    If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
    $endgroup$
    – Kavi Rama Murthy
    Mar 11 at 8:49















0












$begingroup$

Just you polar coordinates and consider the cases $n$ even and $n$ odd separately. The integral is convergent in both cases.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
    $endgroup$
    – C. Bishop
    Mar 11 at 8:48










  • $begingroup$
    If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
    $endgroup$
    – Kavi Rama Murthy
    Mar 11 at 8:49













0












0








0





$begingroup$

Just you polar coordinates and consider the cases $n$ even and $n$ odd separately. The integral is convergent in both cases.






share|cite|improve this answer









$endgroup$



Just you polar coordinates and consider the cases $n$ even and $n$ odd separately. The integral is convergent in both cases.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Mar 11 at 8:44









Kavi Rama MurthyKavi Rama Murthy

67.2k53067




67.2k53067











  • $begingroup$
    I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
    $endgroup$
    – C. Bishop
    Mar 11 at 8:48










  • $begingroup$
    If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
    $endgroup$
    – Kavi Rama Murthy
    Mar 11 at 8:49
















  • $begingroup$
    I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
    $endgroup$
    – C. Bishop
    Mar 11 at 8:48










  • $begingroup$
    If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
    $endgroup$
    – Kavi Rama Murthy
    Mar 11 at 8:49















$begingroup$
I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
$endgroup$
– C. Bishop
Mar 11 at 8:48




$begingroup$
I have no idea from where to start with polar coordinates. Can you help me with the setting up please?
$endgroup$
– C. Bishop
Mar 11 at 8:48












$begingroup$
If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
$endgroup$
– Kavi Rama Murthy
Mar 11 at 8:49




$begingroup$
If you are not familiar with polar coordinate in $mathbb R^n$ you can look at Rudin's RCA.
$endgroup$
– Kavi Rama Murthy
Mar 11 at 8:49



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