Does $sum_{n=1}^infty frac{cos{(sqrt{n})}}{n}$ converge?












17












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The series is:
$$sum_{n=1}^infty frac{cos(sqrt{n})}{n}$$



Considering it isn't always positive, I replace $frac{cos{sqrt{n}}}{n}$ with its absolute value and I find that:
$$vert frac{cos{sqrt{n}}}{n}vertgt frac{cos^2{sqrt{n}}}{n}=frac{ 1+cos{2sqrt{n}}}{2n}=frac{1}{2n}+frac{cos{2sqrt{n}}}{2n}$$
if $sum_{n=1}^infty vertfrac{cos{sqrt{n}}}{n}vert $ converges, then
$sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges.Using Comparison test,we can draw the conclusion that $sum_{n=1}^inftyfrac{1}{2n}$ converges , which is impossible.
So I get that $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ absolutely diverges. But I can't figure out whether $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges or not.



I have tried Dirichlet's test, but I can't figure out whether $$S_{n}=sum_{k=1}^n cos{sqrt{k}}$$ is bounded.



(This is my first time to ask question.Maybe there exist some mistakes in my conclusion.Thanks. :)










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$endgroup$












  • $begingroup$
    If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:27












  • $begingroup$
    Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:32
















17












$begingroup$


The series is:
$$sum_{n=1}^infty frac{cos(sqrt{n})}{n}$$



Considering it isn't always positive, I replace $frac{cos{sqrt{n}}}{n}$ with its absolute value and I find that:
$$vert frac{cos{sqrt{n}}}{n}vertgt frac{cos^2{sqrt{n}}}{n}=frac{ 1+cos{2sqrt{n}}}{2n}=frac{1}{2n}+frac{cos{2sqrt{n}}}{2n}$$
if $sum_{n=1}^infty vertfrac{cos{sqrt{n}}}{n}vert $ converges, then
$sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges.Using Comparison test,we can draw the conclusion that $sum_{n=1}^inftyfrac{1}{2n}$ converges , which is impossible.
So I get that $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ absolutely diverges. But I can't figure out whether $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges or not.



I have tried Dirichlet's test, but I can't figure out whether $$S_{n}=sum_{k=1}^n cos{sqrt{k}}$$ is bounded.



(This is my first time to ask question.Maybe there exist some mistakes in my conclusion.Thanks. :)










share|cite|improve this question











$endgroup$












  • $begingroup$
    If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:27












  • $begingroup$
    Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:32














17












17








17


7



$begingroup$


The series is:
$$sum_{n=1}^infty frac{cos(sqrt{n})}{n}$$



Considering it isn't always positive, I replace $frac{cos{sqrt{n}}}{n}$ with its absolute value and I find that:
$$vert frac{cos{sqrt{n}}}{n}vertgt frac{cos^2{sqrt{n}}}{n}=frac{ 1+cos{2sqrt{n}}}{2n}=frac{1}{2n}+frac{cos{2sqrt{n}}}{2n}$$
if $sum_{n=1}^infty vertfrac{cos{sqrt{n}}}{n}vert $ converges, then
$sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges.Using Comparison test,we can draw the conclusion that $sum_{n=1}^inftyfrac{1}{2n}$ converges , which is impossible.
So I get that $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ absolutely diverges. But I can't figure out whether $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges or not.



I have tried Dirichlet's test, but I can't figure out whether $$S_{n}=sum_{k=1}^n cos{sqrt{k}}$$ is bounded.



(This is my first time to ask question.Maybe there exist some mistakes in my conclusion.Thanks. :)










share|cite|improve this question











$endgroup$




The series is:
$$sum_{n=1}^infty frac{cos(sqrt{n})}{n}$$



Considering it isn't always positive, I replace $frac{cos{sqrt{n}}}{n}$ with its absolute value and I find that:
$$vert frac{cos{sqrt{n}}}{n}vertgt frac{cos^2{sqrt{n}}}{n}=frac{ 1+cos{2sqrt{n}}}{2n}=frac{1}{2n}+frac{cos{2sqrt{n}}}{2n}$$
if $sum_{n=1}^infty vertfrac{cos{sqrt{n}}}{n}vert $ converges, then
$sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges.Using Comparison test,we can draw the conclusion that $sum_{n=1}^inftyfrac{1}{2n}$ converges , which is impossible.
So I get that $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ absolutely diverges. But I can't figure out whether $sum_{n=1}^infty frac{cos{sqrt{n}}}{n}$ converges or not.



I have tried Dirichlet's test, but I can't figure out whether $$S_{n}=sum_{k=1}^n cos{sqrt{k}}$$ is bounded.



(This is my first time to ask question.Maybe there exist some mistakes in my conclusion.Thanks. :)







sequences-and-series analysis trigonometry






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edited Oct 9 '18 at 12:22









Robert Z

101k1071144




101k1071144










asked Oct 9 '18 at 10:53









hmtbgchmtbgc

1097




1097












  • $begingroup$
    If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:27












  • $begingroup$
    Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:32


















  • $begingroup$
    If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:27












  • $begingroup$
    Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
    $endgroup$
    – Batominovski
    Oct 9 '18 at 11:32
















$begingroup$
If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
$endgroup$
– Batominovski
Oct 9 '18 at 11:27






$begingroup$
If you approximate the sum by an integral, then you have $$sum_{n=1}^m,frac{cos(sqrt{n})}{n}approx int_1^m,frac{cos(sqrt{x})}{x},text{d}x=2,text{Ci}(sqrt{m})-2,text{Ci}(1),,$$ where $text{Ci}$ is the cosine integral $$text{Ci}(t)=-int_t^infty,frac{cos(s)}{s},text{d}s,.$$ However, I do not know how accurate the approximation is. But I am convinced that the sum converges since $$lim_{mtoinfty},text{Ci}(sqrt{m})=0,.$$
$endgroup$
– Batominovski
Oct 9 '18 at 11:27














$begingroup$
Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
$endgroup$
– Batominovski
Oct 9 '18 at 11:32




$begingroup$
Plus, after trying to sum up to $3000$ terms, it seems to me that the sum fluctuates around $-0.32$. This looks very promising that the sum does converge to a limit around $-0.32$.
$endgroup$
– Batominovski
Oct 9 '18 at 11:32










5 Answers
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14












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We show that $Ntosum_{n = 1}^N {frac{cos(sqrt{n})}{n}}$ is a Cauchy sequence and therefore the given series is convergent.



Hint. By using the MVT prove that for $ngeq 1$ and for all $xin [n,n+1)$
$$left|frac{cos(sqrt{n})}{n}-frac{cos(sqrt{x})}{x}right|leq frac{1}{n^{3/2}}.$$
Then for $M>Ngeq 1$,
$$begin{align}
&left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - int_N^{M + 1} {frac{{cos (sqrt{x} )}}{x}dx} right|\
&=left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - sum_{n = N}^M {int_n^{n + 1} {frac{{cos (sqrt{x} )}}{x}dx} } right|\
&leqsum_{n = N}^M int_n^{n + 1}left|{frac{cos(sqrt{n})}{n}} - { {frac{{cos (sqrt{x} )}}{x}} } right|dx le sum_{n = N}^M frac{1}{n^{3/2}}.end{align}$$

Note that since $sum_{n=1}^{infty}frac{1}{n^{3/2}}$ is convergent then
$$lim_{M,Nto +infty} sum_{n = N}^M frac{1}{n^{3/2}}=0.$$
Moreover
$$int_1^{+infty}frac{{cos (sqrt{x} )}}{x}dx=2int_1^{+infty}frac{{cos (u )}}{u}, du$$
where the last integral is convergent, and we have that
$$lim_{M,Nto +infty}int_N^{M+1}frac{{cos (sqrt{x} )}}{x}dx=0.$$






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  • $begingroup$
    So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
    $endgroup$
    – Parcly Taxel
    Oct 9 '18 at 11:49










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    Not sure how the first inequality can lead to the second one.
    $endgroup$
    – Szeto
    Oct 9 '18 at 11:50










  • $begingroup$
    @Szeto Is it clear now?
    $endgroup$
    – Robert Z
    Oct 9 '18 at 11:55










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    Thanks for your excellent proof!
    $endgroup$
    – hmtbgc
    Oct 9 '18 at 12:55



















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Not a theoretical answer but a computational one. Ran a SageMath code to check the sum. It appears that the sum is bounded between oscillates in the neighbourhood of $1/3$.



n = 1
s = 0
s_min = s_max = -0.33

while(n < 10^12):
s = s + cos(n^0.5)/n
if(s < s_min):
s_min = s
if(s > s_max):
s_max = s
if(n%10^6 == 0):
print(n,s,s_min,s_max)
n = n + 1


Given below is the sum of the first 540 million terms. I will keep updating the sum after every 100 million terms to see if and where it shows hints of convergence. Looking at these numbers, I wonder if the sum oscillates between -0.3307 and 0.3306.



     n             s_n     
(537000000, -0.330621546932186)
(538000000, -0.330725062788227)
(539000000, -0.330687353946068)
(540000000, -0.330649408748269)
(541000000, -0.330757389552252)
(542000000, -0.330602401857676)
(543000000, -0.330766627976051)
(544000000, -0.330637600125639)
(545000000, -0.330692819220692)
(546000000, -0.330730454234348)
(547000000, -0.330610479504947)
(548000000, -0.330771768297931)
(549000000, -0.330629435680553)
(550000000, -0.330695312033157)
(551000000, -0.330735165460147)
(552000000, -0.330605859570737)
(553000000, -0.330764635324360)
(554000000, -0.330655186664157)





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  • $begingroup$
    A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
    $endgroup$
    – Winther
    Oct 9 '18 at 12:01






  • 1




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    Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
    $endgroup$
    – Dr. Wolfgang Hintze
    Oct 9 '18 at 14:10










  • $begingroup$
    Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
    $endgroup$
    – Mariusz Iwaniuk
    Oct 24 '18 at 17:42





















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Notations: $lfloor x rfloor$ is the floor function, ${x}$ is the fractional part of $x$ so that $x=lfloor xrfloor + {x}$.



Applying partial summation with $f(x)=frac{cos(sqrt x)}x$,
$$begin{align}
sum_{n=1}^N frac{cos(sqrt n)}n&=int_{1-}^N f(x)dlfloor x rfloor \
&=f(x)lfloor xrfloor Bigvert_{1-}^N-int_{1-}^N f'(x)lfloor xrfloor dx\
&=f(N)(N-{N})-int_1^N xf'(x)dx+int_1^N{x}f'(x)dx\
&=Nf(N)-f(1)-int_1^Nxf'(x)dx+int_1^N{x}f'(x)dx+f(1)-{N}f(N).
end{align}
$$

From integration by parts, the sum of first three terms is
$$
int_1^{N}f(x)dx
$$

Thus, we have the following as $Nrightarrowinfty$,
$$
sum_{n=1}^{infty}frac{cos(sqrt n)}n=int_1^{infty}f(x)dx+int_1^{infty}{x}f'(x)dx+cos 1.
$$

It is easy to see that the integrals converge.






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  • $begingroup$
    @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
    $endgroup$
    – Dr. Wolfgang Hintze
    Oct 10 '18 at 13:06












  • $begingroup$
    $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
    $endgroup$
    – i707107
    Oct 11 '18 at 2:13










  • $begingroup$
    Also, you can refer to Riemann-Stieltjes integral.
    $endgroup$
    – i707107
    Oct 11 '18 at 2:14



















1












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This development is similar to that of user i707107 but it is more detailed and avoids the strange expression $d lfloor x rfloor$.



Letting



$$c_{k} = c(k) = frac{cos(sqrt{k})}{k}$$



we attempt to find an integral representation for the partial sum



$$s_n = sum_{k=1}^n c_{k}$$



The formulas for partial summation are



$$sum_{k=1}^n a_{k} b_{k} = A_{n} b_{n} + sum_{k=1}^{n-1} A_{k}(b_{k}-b_{k+1})$$



$$A_{k} = sum_{i=1}^k a_{i}$$



Letting $a_{k}=1, b_{k} = c_{k}$ we have $A_{k} = k$.



Now comes the trick which introduces an integral: we have



$$(b_{k}-b_{k+1}) = - int_{k}^{k+1} c'(x);dx$$



and, what's more, the factor $k$ can be incorporated in the integral:



$$k (b_{k}-b_{k+1}) = - k int_{k}^{k+1} c'(x);dx = - int_{k}^{k+1} lfloor xrfloor c'(x);dx $$



Where $lfloor xrfloor$ is the floor function.



Hence, using



$$lfloor xrfloor = x -{x} $$



where ${x}$ is the fractional part of $x$, the partial sum becomes



$$s_{n} = n c_n -sum_{k=1}^{n-1} int_{k}^{k+1} lfloor xrfloor c'(x);dx \
= n c_n -int_{1}^{n} x c'(x);dx + int_{1}^{n} {x} c'(x);dx$$



By partial integration of the first integral the term $n c_{n}$ drops out and we get



$$s_{n} = cos(1) +int_{1}^{n} c(x);dx + int_{1}^{n} {x} c'(x);dx$$



The first integral can be solved explicitly



$$int_{1}^{n} c(x);dx = 2 text{Ci}left(sqrt{n}right)-2 text{Ci}(1)$$



Where $text{Ci}$ is the integral cosine.



The second integral is absolutely convergent and can be very roughly estimated thus (notice that $0le {x} lt 1$)



$$|i_2| = |int_{1}^{n} {x} c'(x),dx| <= int_{1}^{n}| {x} c'(x)|,dx \
<= int_{1}^{n} |{x}| |c'(x)|,dx
<=int_{1}^{n} | c'(x) | ,dx$$



Now



$$| c'(x) | = |frac{cos left(sqrt{x}right)}{x^2}+frac{sin left(sqrt{x}right)}{2 x^{3/2}}| \
leq | frac{sin left(sqrt{x}right)}{2 x^{3/2}}| +|frac{cos left(sqrt{x}right)}{x^2}| leq frac{1}{2 x^{3/2}}+frac{1}{x^2}$$



Hence



$$| i_2| <=int_1^n left(frac{1}{2 x^{3/2}}+frac{1}{x^2}right) , dx = 2-frac{sqrt{n}+1}{n}tag{*}$$



Since $lim_{nto infty } , text{Ci}left(sqrt{n}right)= 0$ the limit of the partial sum is given by



$$s = cos(1) - 2 text{Ci}(1) + lim_{nto infty } ,i_2$$



Observing (*) $s$ remains finite as $ntoinfty$ hence the original sum is convergent. QED.



Remark



A more sophisticated study if the integral $i_2$ might provide better numerical bounds, and even a closed form.






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$endgroup$





















    1












    $begingroup$

    This approach works in two steps and is generally applicable: first it transforms the sum to an alternating sum which then, in the second step, can be studied by the Dirichlet criterion.



    Step 1: Transformation to an alternating sum



    The partial sum in question is



    $$s_n = sum_{k=1}^n c_ktag{1}$$



    where



    $$c_k = frac{cos(sqrt{k})}{k}tag{2}$$



    Now collecting all subsequent summands with the same sign we can write



    $$s_n = sum_{m=0}^M (-1)^m f_mtag{3}$$



    where



    $$f_0 = sum_{k=1}^{lfloor z_{1}rfloor} c_{k}tag{4a}$$



    $$f_{mge 1} = (-1)^m sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} c_{k}tag{4b}$$



    is the sum of terms between two adjacent roots $k=z_m$ and $k=z_{m+1}$ of $c(k) = 0$, and $M$ is some number depending on $n$ which can in principle be specified but it is normally not necessary as it goes to $infty$ together with $n$



    Then, by an appropirate choice of the factor $(-1)^m$, all $f_m$ can be chosen to be positive quantities.



    Step 2: Application of Dirichlet's criterion



    Now we can apply the Dirichlet criterion to (3). This reads now as follows: $s_n$ is convergent if



    (1) $f_m to 0$ for $mtoinfty$

    (2) $f_m$ is monotonous



    ad (1)



    We have for $mge1$



    $$|f_{m}| le g(m)$$



    where we have dropped the $cos$ and have defined



    $$g(m) = sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} frac{1}{k}
    =H_{lfloor z_{m+1} rfloor}-H_{lceil z_{m}rceil-1}tag{5} $$



    Here $H_n$ ist the harmonic number.



    Now the zeroes of $c_{k}$ are given by



    $$z_m = left(pi(m-frac{1}{2})right)^2tag{6}$$



    Dropping Floor and Ceiling in $g(m)$ defines



    $$g_0(m) = H_{z_{m+1}}-H_{z_{m}-1}$$



    Letting ${lfloor x rfloor} to x-1,{lceil x rceil} to x+1 $ defines another function



    $$g_1(m) = H_{z_{m+1}-1}-H_{z_{m}+1-1}$$



    and we have the inequality



    $$g_1(m) lt g(m) lt g_0(m)$$



    Asymptotically this leads, up to $O(frac{1}{m^2})$, to the inequality



    $$frac{2}{m}- frac{1}{pi^2 m^2}< g(m) <frac{2}{m}+frac{1}{pi^2 m^2} $$



    This shows that $f_m$ goes to zero.



    ad (2)



    (to be continued)






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      5 Answers
      5






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      5 Answers
      5






      active

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      active

      oldest

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      14












      $begingroup$

      We show that $Ntosum_{n = 1}^N {frac{cos(sqrt{n})}{n}}$ is a Cauchy sequence and therefore the given series is convergent.



      Hint. By using the MVT prove that for $ngeq 1$ and for all $xin [n,n+1)$
      $$left|frac{cos(sqrt{n})}{n}-frac{cos(sqrt{x})}{x}right|leq frac{1}{n^{3/2}}.$$
      Then for $M>Ngeq 1$,
      $$begin{align}
      &left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - int_N^{M + 1} {frac{{cos (sqrt{x} )}}{x}dx} right|\
      &=left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - sum_{n = N}^M {int_n^{n + 1} {frac{{cos (sqrt{x} )}}{x}dx} } right|\
      &leqsum_{n = N}^M int_n^{n + 1}left|{frac{cos(sqrt{n})}{n}} - { {frac{{cos (sqrt{x} )}}{x}} } right|dx le sum_{n = N}^M frac{1}{n^{3/2}}.end{align}$$

      Note that since $sum_{n=1}^{infty}frac{1}{n^{3/2}}$ is convergent then
      $$lim_{M,Nto +infty} sum_{n = N}^M frac{1}{n^{3/2}}=0.$$
      Moreover
      $$int_1^{+infty}frac{{cos (sqrt{x} )}}{x}dx=2int_1^{+infty}frac{{cos (u )}}{u}, du$$
      where the last integral is convergent, and we have that
      $$lim_{M,Nto +infty}int_N^{M+1}frac{{cos (sqrt{x} )}}{x}dx=0.$$






      share|cite|improve this answer











      $endgroup$













      • $begingroup$
        So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
        $endgroup$
        – Parcly Taxel
        Oct 9 '18 at 11:49










      • $begingroup$
        Not sure how the first inequality can lead to the second one.
        $endgroup$
        – Szeto
        Oct 9 '18 at 11:50










      • $begingroup$
        @Szeto Is it clear now?
        $endgroup$
        – Robert Z
        Oct 9 '18 at 11:55










      • $begingroup$
        Thanks for your excellent proof!
        $endgroup$
        – hmtbgc
        Oct 9 '18 at 12:55
















      14












      $begingroup$

      We show that $Ntosum_{n = 1}^N {frac{cos(sqrt{n})}{n}}$ is a Cauchy sequence and therefore the given series is convergent.



      Hint. By using the MVT prove that for $ngeq 1$ and for all $xin [n,n+1)$
      $$left|frac{cos(sqrt{n})}{n}-frac{cos(sqrt{x})}{x}right|leq frac{1}{n^{3/2}}.$$
      Then for $M>Ngeq 1$,
      $$begin{align}
      &left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - int_N^{M + 1} {frac{{cos (sqrt{x} )}}{x}dx} right|\
      &=left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - sum_{n = N}^M {int_n^{n + 1} {frac{{cos (sqrt{x} )}}{x}dx} } right|\
      &leqsum_{n = N}^M int_n^{n + 1}left|{frac{cos(sqrt{n})}{n}} - { {frac{{cos (sqrt{x} )}}{x}} } right|dx le sum_{n = N}^M frac{1}{n^{3/2}}.end{align}$$

      Note that since $sum_{n=1}^{infty}frac{1}{n^{3/2}}$ is convergent then
      $$lim_{M,Nto +infty} sum_{n = N}^M frac{1}{n^{3/2}}=0.$$
      Moreover
      $$int_1^{+infty}frac{{cos (sqrt{x} )}}{x}dx=2int_1^{+infty}frac{{cos (u )}}{u}, du$$
      where the last integral is convergent, and we have that
      $$lim_{M,Nto +infty}int_N^{M+1}frac{{cos (sqrt{x} )}}{x}dx=0.$$






      share|cite|improve this answer











      $endgroup$













      • $begingroup$
        So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
        $endgroup$
        – Parcly Taxel
        Oct 9 '18 at 11:49










      • $begingroup$
        Not sure how the first inequality can lead to the second one.
        $endgroup$
        – Szeto
        Oct 9 '18 at 11:50










      • $begingroup$
        @Szeto Is it clear now?
        $endgroup$
        – Robert Z
        Oct 9 '18 at 11:55










      • $begingroup$
        Thanks for your excellent proof!
        $endgroup$
        – hmtbgc
        Oct 9 '18 at 12:55














      14












      14








      14





      $begingroup$

      We show that $Ntosum_{n = 1}^N {frac{cos(sqrt{n})}{n}}$ is a Cauchy sequence and therefore the given series is convergent.



      Hint. By using the MVT prove that for $ngeq 1$ and for all $xin [n,n+1)$
      $$left|frac{cos(sqrt{n})}{n}-frac{cos(sqrt{x})}{x}right|leq frac{1}{n^{3/2}}.$$
      Then for $M>Ngeq 1$,
      $$begin{align}
      &left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - int_N^{M + 1} {frac{{cos (sqrt{x} )}}{x}dx} right|\
      &=left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - sum_{n = N}^M {int_n^{n + 1} {frac{{cos (sqrt{x} )}}{x}dx} } right|\
      &leqsum_{n = N}^M int_n^{n + 1}left|{frac{cos(sqrt{n})}{n}} - { {frac{{cos (sqrt{x} )}}{x}} } right|dx le sum_{n = N}^M frac{1}{n^{3/2}}.end{align}$$

      Note that since $sum_{n=1}^{infty}frac{1}{n^{3/2}}$ is convergent then
      $$lim_{M,Nto +infty} sum_{n = N}^M frac{1}{n^{3/2}}=0.$$
      Moreover
      $$int_1^{+infty}frac{{cos (sqrt{x} )}}{x}dx=2int_1^{+infty}frac{{cos (u )}}{u}, du$$
      where the last integral is convergent, and we have that
      $$lim_{M,Nto +infty}int_N^{M+1}frac{{cos (sqrt{x} )}}{x}dx=0.$$






      share|cite|improve this answer











      $endgroup$



      We show that $Ntosum_{n = 1}^N {frac{cos(sqrt{n})}{n}}$ is a Cauchy sequence and therefore the given series is convergent.



      Hint. By using the MVT prove that for $ngeq 1$ and for all $xin [n,n+1)$
      $$left|frac{cos(sqrt{n})}{n}-frac{cos(sqrt{x})}{x}right|leq frac{1}{n^{3/2}}.$$
      Then for $M>Ngeq 1$,
      $$begin{align}
      &left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - int_N^{M + 1} {frac{{cos (sqrt{x} )}}{x}dx} right|\
      &=left|sum_{n = N}^M {frac{cos(sqrt{n})}{n}} - sum_{n = N}^M {int_n^{n + 1} {frac{{cos (sqrt{x} )}}{x}dx} } right|\
      &leqsum_{n = N}^M int_n^{n + 1}left|{frac{cos(sqrt{n})}{n}} - { {frac{{cos (sqrt{x} )}}{x}} } right|dx le sum_{n = N}^M frac{1}{n^{3/2}}.end{align}$$

      Note that since $sum_{n=1}^{infty}frac{1}{n^{3/2}}$ is convergent then
      $$lim_{M,Nto +infty} sum_{n = N}^M frac{1}{n^{3/2}}=0.$$
      Moreover
      $$int_1^{+infty}frac{{cos (sqrt{x} )}}{x}dx=2int_1^{+infty}frac{{cos (u )}}{u}, du$$
      where the last integral is convergent, and we have that
      $$lim_{M,Nto +infty}int_N^{M+1}frac{{cos (sqrt{x} )}}{x}dx=0.$$







      share|cite|improve this answer














      share|cite|improve this answer



      share|cite|improve this answer








      edited Oct 9 '18 at 13:08

























      answered Oct 9 '18 at 11:46









      Robert ZRobert Z

      101k1071144




      101k1071144












      • $begingroup$
        So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
        $endgroup$
        – Parcly Taxel
        Oct 9 '18 at 11:49










      • $begingroup$
        Not sure how the first inequality can lead to the second one.
        $endgroup$
        – Szeto
        Oct 9 '18 at 11:50










      • $begingroup$
        @Szeto Is it clear now?
        $endgroup$
        – Robert Z
        Oct 9 '18 at 11:55










      • $begingroup$
        Thanks for your excellent proof!
        $endgroup$
        – hmtbgc
        Oct 9 '18 at 12:55


















      • $begingroup$
        So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
        $endgroup$
        – Parcly Taxel
        Oct 9 '18 at 11:49










      • $begingroup$
        Not sure how the first inequality can lead to the second one.
        $endgroup$
        – Szeto
        Oct 9 '18 at 11:50










      • $begingroup$
        @Szeto Is it clear now?
        $endgroup$
        – Robert Z
        Oct 9 '18 at 11:55










      • $begingroup$
        Thanks for your excellent proof!
        $endgroup$
        – hmtbgc
        Oct 9 '18 at 12:55
















      $begingroup$
      So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
      $endgroup$
      – Parcly Taxel
      Oct 9 '18 at 11:49




      $begingroup$
      So ultimately the absolute-term series is less than $zeta(3/2)$ and thus the original series converges?
      $endgroup$
      – Parcly Taxel
      Oct 9 '18 at 11:49












      $begingroup$
      Not sure how the first inequality can lead to the second one.
      $endgroup$
      – Szeto
      Oct 9 '18 at 11:50




      $begingroup$
      Not sure how the first inequality can lead to the second one.
      $endgroup$
      – Szeto
      Oct 9 '18 at 11:50












      $begingroup$
      @Szeto Is it clear now?
      $endgroup$
      – Robert Z
      Oct 9 '18 at 11:55




      $begingroup$
      @Szeto Is it clear now?
      $endgroup$
      – Robert Z
      Oct 9 '18 at 11:55












      $begingroup$
      Thanks for your excellent proof!
      $endgroup$
      – hmtbgc
      Oct 9 '18 at 12:55




      $begingroup$
      Thanks for your excellent proof!
      $endgroup$
      – hmtbgc
      Oct 9 '18 at 12:55











      3












      $begingroup$

      Not a theoretical answer but a computational one. Ran a SageMath code to check the sum. It appears that the sum is bounded between oscillates in the neighbourhood of $1/3$.



      n = 1
      s = 0
      s_min = s_max = -0.33

      while(n < 10^12):
      s = s + cos(n^0.5)/n
      if(s < s_min):
      s_min = s
      if(s > s_max):
      s_max = s
      if(n%10^6 == 0):
      print(n,s,s_min,s_max)
      n = n + 1


      Given below is the sum of the first 540 million terms. I will keep updating the sum after every 100 million terms to see if and where it shows hints of convergence. Looking at these numbers, I wonder if the sum oscillates between -0.3307 and 0.3306.



           n             s_n     
      (537000000, -0.330621546932186)
      (538000000, -0.330725062788227)
      (539000000, -0.330687353946068)
      (540000000, -0.330649408748269)
      (541000000, -0.330757389552252)
      (542000000, -0.330602401857676)
      (543000000, -0.330766627976051)
      (544000000, -0.330637600125639)
      (545000000, -0.330692819220692)
      (546000000, -0.330730454234348)
      (547000000, -0.330610479504947)
      (548000000, -0.330771768297931)
      (549000000, -0.330629435680553)
      (550000000, -0.330695312033157)
      (551000000, -0.330735165460147)
      (552000000, -0.330605859570737)
      (553000000, -0.330764635324360)
      (554000000, -0.330655186664157)





      share|cite|improve this answer











      $endgroup$













      • $begingroup$
        A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
        $endgroup$
        – Winther
        Oct 9 '18 at 12:01






      • 1




        $begingroup$
        Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 9 '18 at 14:10










      • $begingroup$
        Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
        $endgroup$
        – Mariusz Iwaniuk
        Oct 24 '18 at 17:42


















      3












      $begingroup$

      Not a theoretical answer but a computational one. Ran a SageMath code to check the sum. It appears that the sum is bounded between oscillates in the neighbourhood of $1/3$.



      n = 1
      s = 0
      s_min = s_max = -0.33

      while(n < 10^12):
      s = s + cos(n^0.5)/n
      if(s < s_min):
      s_min = s
      if(s > s_max):
      s_max = s
      if(n%10^6 == 0):
      print(n,s,s_min,s_max)
      n = n + 1


      Given below is the sum of the first 540 million terms. I will keep updating the sum after every 100 million terms to see if and where it shows hints of convergence. Looking at these numbers, I wonder if the sum oscillates between -0.3307 and 0.3306.



           n             s_n     
      (537000000, -0.330621546932186)
      (538000000, -0.330725062788227)
      (539000000, -0.330687353946068)
      (540000000, -0.330649408748269)
      (541000000, -0.330757389552252)
      (542000000, -0.330602401857676)
      (543000000, -0.330766627976051)
      (544000000, -0.330637600125639)
      (545000000, -0.330692819220692)
      (546000000, -0.330730454234348)
      (547000000, -0.330610479504947)
      (548000000, -0.330771768297931)
      (549000000, -0.330629435680553)
      (550000000, -0.330695312033157)
      (551000000, -0.330735165460147)
      (552000000, -0.330605859570737)
      (553000000, -0.330764635324360)
      (554000000, -0.330655186664157)





      share|cite|improve this answer











      $endgroup$













      • $begingroup$
        A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
        $endgroup$
        – Winther
        Oct 9 '18 at 12:01






      • 1




        $begingroup$
        Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 9 '18 at 14:10










      • $begingroup$
        Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
        $endgroup$
        – Mariusz Iwaniuk
        Oct 24 '18 at 17:42
















      3












      3








      3





      $begingroup$

      Not a theoretical answer but a computational one. Ran a SageMath code to check the sum. It appears that the sum is bounded between oscillates in the neighbourhood of $1/3$.



      n = 1
      s = 0
      s_min = s_max = -0.33

      while(n < 10^12):
      s = s + cos(n^0.5)/n
      if(s < s_min):
      s_min = s
      if(s > s_max):
      s_max = s
      if(n%10^6 == 0):
      print(n,s,s_min,s_max)
      n = n + 1


      Given below is the sum of the first 540 million terms. I will keep updating the sum after every 100 million terms to see if and where it shows hints of convergence. Looking at these numbers, I wonder if the sum oscillates between -0.3307 and 0.3306.



           n             s_n     
      (537000000, -0.330621546932186)
      (538000000, -0.330725062788227)
      (539000000, -0.330687353946068)
      (540000000, -0.330649408748269)
      (541000000, -0.330757389552252)
      (542000000, -0.330602401857676)
      (543000000, -0.330766627976051)
      (544000000, -0.330637600125639)
      (545000000, -0.330692819220692)
      (546000000, -0.330730454234348)
      (547000000, -0.330610479504947)
      (548000000, -0.330771768297931)
      (549000000, -0.330629435680553)
      (550000000, -0.330695312033157)
      (551000000, -0.330735165460147)
      (552000000, -0.330605859570737)
      (553000000, -0.330764635324360)
      (554000000, -0.330655186664157)





      share|cite|improve this answer











      $endgroup$



      Not a theoretical answer but a computational one. Ran a SageMath code to check the sum. It appears that the sum is bounded between oscillates in the neighbourhood of $1/3$.



      n = 1
      s = 0
      s_min = s_max = -0.33

      while(n < 10^12):
      s = s + cos(n^0.5)/n
      if(s < s_min):
      s_min = s
      if(s > s_max):
      s_max = s
      if(n%10^6 == 0):
      print(n,s,s_min,s_max)
      n = n + 1


      Given below is the sum of the first 540 million terms. I will keep updating the sum after every 100 million terms to see if and where it shows hints of convergence. Looking at these numbers, I wonder if the sum oscillates between -0.3307 and 0.3306.



           n             s_n     
      (537000000, -0.330621546932186)
      (538000000, -0.330725062788227)
      (539000000, -0.330687353946068)
      (540000000, -0.330649408748269)
      (541000000, -0.330757389552252)
      (542000000, -0.330602401857676)
      (543000000, -0.330766627976051)
      (544000000, -0.330637600125639)
      (545000000, -0.330692819220692)
      (546000000, -0.330730454234348)
      (547000000, -0.330610479504947)
      (548000000, -0.330771768297931)
      (549000000, -0.330629435680553)
      (550000000, -0.330695312033157)
      (551000000, -0.330735165460147)
      (552000000, -0.330605859570737)
      (553000000, -0.330764635324360)
      (554000000, -0.330655186664157)






      share|cite|improve this answer














      share|cite|improve this answer



      share|cite|improve this answer








      edited Oct 9 '18 at 15:37

























      answered Oct 9 '18 at 11:40









      Nilotpal Kanti SinhaNilotpal Kanti Sinha

      4,43021640




      4,43021640












      • $begingroup$
        A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
        $endgroup$
        – Winther
        Oct 9 '18 at 12:01






      • 1




        $begingroup$
        Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 9 '18 at 14:10










      • $begingroup$
        Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
        $endgroup$
        – Mariusz Iwaniuk
        Oct 24 '18 at 17:42




















      • $begingroup$
        A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
        $endgroup$
        – Winther
        Oct 9 '18 at 12:01






      • 1




        $begingroup$
        Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 9 '18 at 14:10










      • $begingroup$
        Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
        $endgroup$
        – Mariusz Iwaniuk
        Oct 24 '18 at 17:42


















      $begingroup$
      A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
      $endgroup$
      – Winther
      Oct 9 '18 at 12:01




      $begingroup$
      A quick estimate suggest you roughly need $sim 10^{2k}$ terms to get convergence to $k$ digits.
      $endgroup$
      – Winther
      Oct 9 '18 at 12:01




      1




      1




      $begingroup$
      Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
      $endgroup$
      – Dr. Wolfgang Hintze
      Oct 9 '18 at 14:10




      $begingroup$
      Letting $a(k) = frac{cos left(sqrt{k}right)}{k}$ Mathematica gives $s=text{NSum[a[k], {k, 1, infty}]} = -0.330688$
      $endgroup$
      – Dr. Wolfgang Hintze
      Oct 9 '18 at 14:10












      $begingroup$
      Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
      $endgroup$
      – Mariusz Iwaniuk
      Oct 24 '18 at 17:42






      $begingroup$
      Numeric inverse Laplace: $gamma +mathcal{L}_s^{-1}left[frac{psi left(1+s^2right)}{s}right](1)approx -0.33068768045214513116891754615748$ where $psi$ is PolyGamma and $gamma$ is EulerGamma.
      $endgroup$
      – Mariusz Iwaniuk
      Oct 24 '18 at 17:42













      2












      $begingroup$

      Notations: $lfloor x rfloor$ is the floor function, ${x}$ is the fractional part of $x$ so that $x=lfloor xrfloor + {x}$.



      Applying partial summation with $f(x)=frac{cos(sqrt x)}x$,
      $$begin{align}
      sum_{n=1}^N frac{cos(sqrt n)}n&=int_{1-}^N f(x)dlfloor x rfloor \
      &=f(x)lfloor xrfloor Bigvert_{1-}^N-int_{1-}^N f'(x)lfloor xrfloor dx\
      &=f(N)(N-{N})-int_1^N xf'(x)dx+int_1^N{x}f'(x)dx\
      &=Nf(N)-f(1)-int_1^Nxf'(x)dx+int_1^N{x}f'(x)dx+f(1)-{N}f(N).
      end{align}
      $$

      From integration by parts, the sum of first three terms is
      $$
      int_1^{N}f(x)dx
      $$

      Thus, we have the following as $Nrightarrowinfty$,
      $$
      sum_{n=1}^{infty}frac{cos(sqrt n)}n=int_1^{infty}f(x)dx+int_1^{infty}{x}f'(x)dx+cos 1.
      $$

      It is easy to see that the integrals converge.






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 10 '18 at 13:06












      • $begingroup$
        $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:13










      • $begingroup$
        Also, you can refer to Riemann-Stieltjes integral.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:14
















      2












      $begingroup$

      Notations: $lfloor x rfloor$ is the floor function, ${x}$ is the fractional part of $x$ so that $x=lfloor xrfloor + {x}$.



      Applying partial summation with $f(x)=frac{cos(sqrt x)}x$,
      $$begin{align}
      sum_{n=1}^N frac{cos(sqrt n)}n&=int_{1-}^N f(x)dlfloor x rfloor \
      &=f(x)lfloor xrfloor Bigvert_{1-}^N-int_{1-}^N f'(x)lfloor xrfloor dx\
      &=f(N)(N-{N})-int_1^N xf'(x)dx+int_1^N{x}f'(x)dx\
      &=Nf(N)-f(1)-int_1^Nxf'(x)dx+int_1^N{x}f'(x)dx+f(1)-{N}f(N).
      end{align}
      $$

      From integration by parts, the sum of first three terms is
      $$
      int_1^{N}f(x)dx
      $$

      Thus, we have the following as $Nrightarrowinfty$,
      $$
      sum_{n=1}^{infty}frac{cos(sqrt n)}n=int_1^{infty}f(x)dx+int_1^{infty}{x}f'(x)dx+cos 1.
      $$

      It is easy to see that the integrals converge.






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 10 '18 at 13:06












      • $begingroup$
        $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:13










      • $begingroup$
        Also, you can refer to Riemann-Stieltjes integral.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:14














      2












      2








      2





      $begingroup$

      Notations: $lfloor x rfloor$ is the floor function, ${x}$ is the fractional part of $x$ so that $x=lfloor xrfloor + {x}$.



      Applying partial summation with $f(x)=frac{cos(sqrt x)}x$,
      $$begin{align}
      sum_{n=1}^N frac{cos(sqrt n)}n&=int_{1-}^N f(x)dlfloor x rfloor \
      &=f(x)lfloor xrfloor Bigvert_{1-}^N-int_{1-}^N f'(x)lfloor xrfloor dx\
      &=f(N)(N-{N})-int_1^N xf'(x)dx+int_1^N{x}f'(x)dx\
      &=Nf(N)-f(1)-int_1^Nxf'(x)dx+int_1^N{x}f'(x)dx+f(1)-{N}f(N).
      end{align}
      $$

      From integration by parts, the sum of first three terms is
      $$
      int_1^{N}f(x)dx
      $$

      Thus, we have the following as $Nrightarrowinfty$,
      $$
      sum_{n=1}^{infty}frac{cos(sqrt n)}n=int_1^{infty}f(x)dx+int_1^{infty}{x}f'(x)dx+cos 1.
      $$

      It is easy to see that the integrals converge.






      share|cite|improve this answer









      $endgroup$



      Notations: $lfloor x rfloor$ is the floor function, ${x}$ is the fractional part of $x$ so that $x=lfloor xrfloor + {x}$.



      Applying partial summation with $f(x)=frac{cos(sqrt x)}x$,
      $$begin{align}
      sum_{n=1}^N frac{cos(sqrt n)}n&=int_{1-}^N f(x)dlfloor x rfloor \
      &=f(x)lfloor xrfloor Bigvert_{1-}^N-int_{1-}^N f'(x)lfloor xrfloor dx\
      &=f(N)(N-{N})-int_1^N xf'(x)dx+int_1^N{x}f'(x)dx\
      &=Nf(N)-f(1)-int_1^Nxf'(x)dx+int_1^N{x}f'(x)dx+f(1)-{N}f(N).
      end{align}
      $$

      From integration by parts, the sum of first three terms is
      $$
      int_1^{N}f(x)dx
      $$

      Thus, we have the following as $Nrightarrowinfty$,
      $$
      sum_{n=1}^{infty}frac{cos(sqrt n)}n=int_1^{infty}f(x)dx+int_1^{infty}{x}f'(x)dx+cos 1.
      $$

      It is easy to see that the integrals converge.







      share|cite|improve this answer












      share|cite|improve this answer



      share|cite|improve this answer










      answered Oct 10 '18 at 5:08









      i707107i707107

      12.6k21647




      12.6k21647












      • $begingroup$
        @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 10 '18 at 13:06












      • $begingroup$
        $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:13










      • $begingroup$
        Also, you can refer to Riemann-Stieltjes integral.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:14


















      • $begingroup$
        @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
        $endgroup$
        – Dr. Wolfgang Hintze
        Oct 10 '18 at 13:06












      • $begingroup$
        $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:13










      • $begingroup$
        Also, you can refer to Riemann-Stieltjes integral.
        $endgroup$
        – i707107
        Oct 11 '18 at 2:14
















      $begingroup$
      @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
      $endgroup$
      – Dr. Wolfgang Hintze
      Oct 10 '18 at 13:06






      $begingroup$
      @ i707107 I have derived the same final formula, but without using the differential $dlfloor xrfloor$ which looks strange to me. Could you please explain its meaning.
      $endgroup$
      – Dr. Wolfgang Hintze
      Oct 10 '18 at 13:06














      $begingroup$
      $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
      $endgroup$
      – i707107
      Oct 11 '18 at 2:13




      $begingroup$
      $dlfloor xrfloor$ means that you take the jump amount whenever there is a jump. The jumps of $lfloor x rfloor$ occur at integers with amount $1$. So, the integral on the right in fact means the same as the sum on the left. The formula I use is a partial summation formula, this is Abel's summation formula in wikipedia.
      $endgroup$
      – i707107
      Oct 11 '18 at 2:13












      $begingroup$
      Also, you can refer to Riemann-Stieltjes integral.
      $endgroup$
      – i707107
      Oct 11 '18 at 2:14




      $begingroup$
      Also, you can refer to Riemann-Stieltjes integral.
      $endgroup$
      – i707107
      Oct 11 '18 at 2:14











      1












      $begingroup$

      This development is similar to that of user i707107 but it is more detailed and avoids the strange expression $d lfloor x rfloor$.



      Letting



      $$c_{k} = c(k) = frac{cos(sqrt{k})}{k}$$



      we attempt to find an integral representation for the partial sum



      $$s_n = sum_{k=1}^n c_{k}$$



      The formulas for partial summation are



      $$sum_{k=1}^n a_{k} b_{k} = A_{n} b_{n} + sum_{k=1}^{n-1} A_{k}(b_{k}-b_{k+1})$$



      $$A_{k} = sum_{i=1}^k a_{i}$$



      Letting $a_{k}=1, b_{k} = c_{k}$ we have $A_{k} = k$.



      Now comes the trick which introduces an integral: we have



      $$(b_{k}-b_{k+1}) = - int_{k}^{k+1} c'(x);dx$$



      and, what's more, the factor $k$ can be incorporated in the integral:



      $$k (b_{k}-b_{k+1}) = - k int_{k}^{k+1} c'(x);dx = - int_{k}^{k+1} lfloor xrfloor c'(x);dx $$



      Where $lfloor xrfloor$ is the floor function.



      Hence, using



      $$lfloor xrfloor = x -{x} $$



      where ${x}$ is the fractional part of $x$, the partial sum becomes



      $$s_{n} = n c_n -sum_{k=1}^{n-1} int_{k}^{k+1} lfloor xrfloor c'(x);dx \
      = n c_n -int_{1}^{n} x c'(x);dx + int_{1}^{n} {x} c'(x);dx$$



      By partial integration of the first integral the term $n c_{n}$ drops out and we get



      $$s_{n} = cos(1) +int_{1}^{n} c(x);dx + int_{1}^{n} {x} c'(x);dx$$



      The first integral can be solved explicitly



      $$int_{1}^{n} c(x);dx = 2 text{Ci}left(sqrt{n}right)-2 text{Ci}(1)$$



      Where $text{Ci}$ is the integral cosine.



      The second integral is absolutely convergent and can be very roughly estimated thus (notice that $0le {x} lt 1$)



      $$|i_2| = |int_{1}^{n} {x} c'(x),dx| <= int_{1}^{n}| {x} c'(x)|,dx \
      <= int_{1}^{n} |{x}| |c'(x)|,dx
      <=int_{1}^{n} | c'(x) | ,dx$$



      Now



      $$| c'(x) | = |frac{cos left(sqrt{x}right)}{x^2}+frac{sin left(sqrt{x}right)}{2 x^{3/2}}| \
      leq | frac{sin left(sqrt{x}right)}{2 x^{3/2}}| +|frac{cos left(sqrt{x}right)}{x^2}| leq frac{1}{2 x^{3/2}}+frac{1}{x^2}$$



      Hence



      $$| i_2| <=int_1^n left(frac{1}{2 x^{3/2}}+frac{1}{x^2}right) , dx = 2-frac{sqrt{n}+1}{n}tag{*}$$



      Since $lim_{nto infty } , text{Ci}left(sqrt{n}right)= 0$ the limit of the partial sum is given by



      $$s = cos(1) - 2 text{Ci}(1) + lim_{nto infty } ,i_2$$



      Observing (*) $s$ remains finite as $ntoinfty$ hence the original sum is convergent. QED.



      Remark



      A more sophisticated study if the integral $i_2$ might provide better numerical bounds, and even a closed form.






      share|cite|improve this answer











      $endgroup$


















        1












        $begingroup$

        This development is similar to that of user i707107 but it is more detailed and avoids the strange expression $d lfloor x rfloor$.



        Letting



        $$c_{k} = c(k) = frac{cos(sqrt{k})}{k}$$



        we attempt to find an integral representation for the partial sum



        $$s_n = sum_{k=1}^n c_{k}$$



        The formulas for partial summation are



        $$sum_{k=1}^n a_{k} b_{k} = A_{n} b_{n} + sum_{k=1}^{n-1} A_{k}(b_{k}-b_{k+1})$$



        $$A_{k} = sum_{i=1}^k a_{i}$$



        Letting $a_{k}=1, b_{k} = c_{k}$ we have $A_{k} = k$.



        Now comes the trick which introduces an integral: we have



        $$(b_{k}-b_{k+1}) = - int_{k}^{k+1} c'(x);dx$$



        and, what's more, the factor $k$ can be incorporated in the integral:



        $$k (b_{k}-b_{k+1}) = - k int_{k}^{k+1} c'(x);dx = - int_{k}^{k+1} lfloor xrfloor c'(x);dx $$



        Where $lfloor xrfloor$ is the floor function.



        Hence, using



        $$lfloor xrfloor = x -{x} $$



        where ${x}$ is the fractional part of $x$, the partial sum becomes



        $$s_{n} = n c_n -sum_{k=1}^{n-1} int_{k}^{k+1} lfloor xrfloor c'(x);dx \
        = n c_n -int_{1}^{n} x c'(x);dx + int_{1}^{n} {x} c'(x);dx$$



        By partial integration of the first integral the term $n c_{n}$ drops out and we get



        $$s_{n} = cos(1) +int_{1}^{n} c(x);dx + int_{1}^{n} {x} c'(x);dx$$



        The first integral can be solved explicitly



        $$int_{1}^{n} c(x);dx = 2 text{Ci}left(sqrt{n}right)-2 text{Ci}(1)$$



        Where $text{Ci}$ is the integral cosine.



        The second integral is absolutely convergent and can be very roughly estimated thus (notice that $0le {x} lt 1$)



        $$|i_2| = |int_{1}^{n} {x} c'(x),dx| <= int_{1}^{n}| {x} c'(x)|,dx \
        <= int_{1}^{n} |{x}| |c'(x)|,dx
        <=int_{1}^{n} | c'(x) | ,dx$$



        Now



        $$| c'(x) | = |frac{cos left(sqrt{x}right)}{x^2}+frac{sin left(sqrt{x}right)}{2 x^{3/2}}| \
        leq | frac{sin left(sqrt{x}right)}{2 x^{3/2}}| +|frac{cos left(sqrt{x}right)}{x^2}| leq frac{1}{2 x^{3/2}}+frac{1}{x^2}$$



        Hence



        $$| i_2| <=int_1^n left(frac{1}{2 x^{3/2}}+frac{1}{x^2}right) , dx = 2-frac{sqrt{n}+1}{n}tag{*}$$



        Since $lim_{nto infty } , text{Ci}left(sqrt{n}right)= 0$ the limit of the partial sum is given by



        $$s = cos(1) - 2 text{Ci}(1) + lim_{nto infty } ,i_2$$



        Observing (*) $s$ remains finite as $ntoinfty$ hence the original sum is convergent. QED.



        Remark



        A more sophisticated study if the integral $i_2$ might provide better numerical bounds, and even a closed form.






        share|cite|improve this answer











        $endgroup$
















          1












          1








          1





          $begingroup$

          This development is similar to that of user i707107 but it is more detailed and avoids the strange expression $d lfloor x rfloor$.



          Letting



          $$c_{k} = c(k) = frac{cos(sqrt{k})}{k}$$



          we attempt to find an integral representation for the partial sum



          $$s_n = sum_{k=1}^n c_{k}$$



          The formulas for partial summation are



          $$sum_{k=1}^n a_{k} b_{k} = A_{n} b_{n} + sum_{k=1}^{n-1} A_{k}(b_{k}-b_{k+1})$$



          $$A_{k} = sum_{i=1}^k a_{i}$$



          Letting $a_{k}=1, b_{k} = c_{k}$ we have $A_{k} = k$.



          Now comes the trick which introduces an integral: we have



          $$(b_{k}-b_{k+1}) = - int_{k}^{k+1} c'(x);dx$$



          and, what's more, the factor $k$ can be incorporated in the integral:



          $$k (b_{k}-b_{k+1}) = - k int_{k}^{k+1} c'(x);dx = - int_{k}^{k+1} lfloor xrfloor c'(x);dx $$



          Where $lfloor xrfloor$ is the floor function.



          Hence, using



          $$lfloor xrfloor = x -{x} $$



          where ${x}$ is the fractional part of $x$, the partial sum becomes



          $$s_{n} = n c_n -sum_{k=1}^{n-1} int_{k}^{k+1} lfloor xrfloor c'(x);dx \
          = n c_n -int_{1}^{n} x c'(x);dx + int_{1}^{n} {x} c'(x);dx$$



          By partial integration of the first integral the term $n c_{n}$ drops out and we get



          $$s_{n} = cos(1) +int_{1}^{n} c(x);dx + int_{1}^{n} {x} c'(x);dx$$



          The first integral can be solved explicitly



          $$int_{1}^{n} c(x);dx = 2 text{Ci}left(sqrt{n}right)-2 text{Ci}(1)$$



          Where $text{Ci}$ is the integral cosine.



          The second integral is absolutely convergent and can be very roughly estimated thus (notice that $0le {x} lt 1$)



          $$|i_2| = |int_{1}^{n} {x} c'(x),dx| <= int_{1}^{n}| {x} c'(x)|,dx \
          <= int_{1}^{n} |{x}| |c'(x)|,dx
          <=int_{1}^{n} | c'(x) | ,dx$$



          Now



          $$| c'(x) | = |frac{cos left(sqrt{x}right)}{x^2}+frac{sin left(sqrt{x}right)}{2 x^{3/2}}| \
          leq | frac{sin left(sqrt{x}right)}{2 x^{3/2}}| +|frac{cos left(sqrt{x}right)}{x^2}| leq frac{1}{2 x^{3/2}}+frac{1}{x^2}$$



          Hence



          $$| i_2| <=int_1^n left(frac{1}{2 x^{3/2}}+frac{1}{x^2}right) , dx = 2-frac{sqrt{n}+1}{n}tag{*}$$



          Since $lim_{nto infty } , text{Ci}left(sqrt{n}right)= 0$ the limit of the partial sum is given by



          $$s = cos(1) - 2 text{Ci}(1) + lim_{nto infty } ,i_2$$



          Observing (*) $s$ remains finite as $ntoinfty$ hence the original sum is convergent. QED.



          Remark



          A more sophisticated study if the integral $i_2$ might provide better numerical bounds, and even a closed form.






          share|cite|improve this answer











          $endgroup$



          This development is similar to that of user i707107 but it is more detailed and avoids the strange expression $d lfloor x rfloor$.



          Letting



          $$c_{k} = c(k) = frac{cos(sqrt{k})}{k}$$



          we attempt to find an integral representation for the partial sum



          $$s_n = sum_{k=1}^n c_{k}$$



          The formulas for partial summation are



          $$sum_{k=1}^n a_{k} b_{k} = A_{n} b_{n} + sum_{k=1}^{n-1} A_{k}(b_{k}-b_{k+1})$$



          $$A_{k} = sum_{i=1}^k a_{i}$$



          Letting $a_{k}=1, b_{k} = c_{k}$ we have $A_{k} = k$.



          Now comes the trick which introduces an integral: we have



          $$(b_{k}-b_{k+1}) = - int_{k}^{k+1} c'(x);dx$$



          and, what's more, the factor $k$ can be incorporated in the integral:



          $$k (b_{k}-b_{k+1}) = - k int_{k}^{k+1} c'(x);dx = - int_{k}^{k+1} lfloor xrfloor c'(x);dx $$



          Where $lfloor xrfloor$ is the floor function.



          Hence, using



          $$lfloor xrfloor = x -{x} $$



          where ${x}$ is the fractional part of $x$, the partial sum becomes



          $$s_{n} = n c_n -sum_{k=1}^{n-1} int_{k}^{k+1} lfloor xrfloor c'(x);dx \
          = n c_n -int_{1}^{n} x c'(x);dx + int_{1}^{n} {x} c'(x);dx$$



          By partial integration of the first integral the term $n c_{n}$ drops out and we get



          $$s_{n} = cos(1) +int_{1}^{n} c(x);dx + int_{1}^{n} {x} c'(x);dx$$



          The first integral can be solved explicitly



          $$int_{1}^{n} c(x);dx = 2 text{Ci}left(sqrt{n}right)-2 text{Ci}(1)$$



          Where $text{Ci}$ is the integral cosine.



          The second integral is absolutely convergent and can be very roughly estimated thus (notice that $0le {x} lt 1$)



          $$|i_2| = |int_{1}^{n} {x} c'(x),dx| <= int_{1}^{n}| {x} c'(x)|,dx \
          <= int_{1}^{n} |{x}| |c'(x)|,dx
          <=int_{1}^{n} | c'(x) | ,dx$$



          Now



          $$| c'(x) | = |frac{cos left(sqrt{x}right)}{x^2}+frac{sin left(sqrt{x}right)}{2 x^{3/2}}| \
          leq | frac{sin left(sqrt{x}right)}{2 x^{3/2}}| +|frac{cos left(sqrt{x}right)}{x^2}| leq frac{1}{2 x^{3/2}}+frac{1}{x^2}$$



          Hence



          $$| i_2| <=int_1^n left(frac{1}{2 x^{3/2}}+frac{1}{x^2}right) , dx = 2-frac{sqrt{n}+1}{n}tag{*}$$



          Since $lim_{nto infty } , text{Ci}left(sqrt{n}right)= 0$ the limit of the partial sum is given by



          $$s = cos(1) - 2 text{Ci}(1) + lim_{nto infty } ,i_2$$



          Observing (*) $s$ remains finite as $ntoinfty$ hence the original sum is convergent. QED.



          Remark



          A more sophisticated study if the integral $i_2$ might provide better numerical bounds, and even a closed form.







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Oct 11 '18 at 11:04

























          answered Oct 10 '18 at 15:06









          Dr. Wolfgang HintzeDr. Wolfgang Hintze

          3,890621




          3,890621























              1












              $begingroup$

              This approach works in two steps and is generally applicable: first it transforms the sum to an alternating sum which then, in the second step, can be studied by the Dirichlet criterion.



              Step 1: Transformation to an alternating sum



              The partial sum in question is



              $$s_n = sum_{k=1}^n c_ktag{1}$$



              where



              $$c_k = frac{cos(sqrt{k})}{k}tag{2}$$



              Now collecting all subsequent summands with the same sign we can write



              $$s_n = sum_{m=0}^M (-1)^m f_mtag{3}$$



              where



              $$f_0 = sum_{k=1}^{lfloor z_{1}rfloor} c_{k}tag{4a}$$



              $$f_{mge 1} = (-1)^m sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} c_{k}tag{4b}$$



              is the sum of terms between two adjacent roots $k=z_m$ and $k=z_{m+1}$ of $c(k) = 0$, and $M$ is some number depending on $n$ which can in principle be specified but it is normally not necessary as it goes to $infty$ together with $n$



              Then, by an appropirate choice of the factor $(-1)^m$, all $f_m$ can be chosen to be positive quantities.



              Step 2: Application of Dirichlet's criterion



              Now we can apply the Dirichlet criterion to (3). This reads now as follows: $s_n$ is convergent if



              (1) $f_m to 0$ for $mtoinfty$

              (2) $f_m$ is monotonous



              ad (1)



              We have for $mge1$



              $$|f_{m}| le g(m)$$



              where we have dropped the $cos$ and have defined



              $$g(m) = sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} frac{1}{k}
              =H_{lfloor z_{m+1} rfloor}-H_{lceil z_{m}rceil-1}tag{5} $$



              Here $H_n$ ist the harmonic number.



              Now the zeroes of $c_{k}$ are given by



              $$z_m = left(pi(m-frac{1}{2})right)^2tag{6}$$



              Dropping Floor and Ceiling in $g(m)$ defines



              $$g_0(m) = H_{z_{m+1}}-H_{z_{m}-1}$$



              Letting ${lfloor x rfloor} to x-1,{lceil x rceil} to x+1 $ defines another function



              $$g_1(m) = H_{z_{m+1}-1}-H_{z_{m}+1-1}$$



              and we have the inequality



              $$g_1(m) lt g(m) lt g_0(m)$$



              Asymptotically this leads, up to $O(frac{1}{m^2})$, to the inequality



              $$frac{2}{m}- frac{1}{pi^2 m^2}< g(m) <frac{2}{m}+frac{1}{pi^2 m^2} $$



              This shows that $f_m$ goes to zero.



              ad (2)



              (to be continued)






              share|cite|improve this answer











              $endgroup$


















                1












                $begingroup$

                This approach works in two steps and is generally applicable: first it transforms the sum to an alternating sum which then, in the second step, can be studied by the Dirichlet criterion.



                Step 1: Transformation to an alternating sum



                The partial sum in question is



                $$s_n = sum_{k=1}^n c_ktag{1}$$



                where



                $$c_k = frac{cos(sqrt{k})}{k}tag{2}$$



                Now collecting all subsequent summands with the same sign we can write



                $$s_n = sum_{m=0}^M (-1)^m f_mtag{3}$$



                where



                $$f_0 = sum_{k=1}^{lfloor z_{1}rfloor} c_{k}tag{4a}$$



                $$f_{mge 1} = (-1)^m sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} c_{k}tag{4b}$$



                is the sum of terms between two adjacent roots $k=z_m$ and $k=z_{m+1}$ of $c(k) = 0$, and $M$ is some number depending on $n$ which can in principle be specified but it is normally not necessary as it goes to $infty$ together with $n$



                Then, by an appropirate choice of the factor $(-1)^m$, all $f_m$ can be chosen to be positive quantities.



                Step 2: Application of Dirichlet's criterion



                Now we can apply the Dirichlet criterion to (3). This reads now as follows: $s_n$ is convergent if



                (1) $f_m to 0$ for $mtoinfty$

                (2) $f_m$ is monotonous



                ad (1)



                We have for $mge1$



                $$|f_{m}| le g(m)$$



                where we have dropped the $cos$ and have defined



                $$g(m) = sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} frac{1}{k}
                =H_{lfloor z_{m+1} rfloor}-H_{lceil z_{m}rceil-1}tag{5} $$



                Here $H_n$ ist the harmonic number.



                Now the zeroes of $c_{k}$ are given by



                $$z_m = left(pi(m-frac{1}{2})right)^2tag{6}$$



                Dropping Floor and Ceiling in $g(m)$ defines



                $$g_0(m) = H_{z_{m+1}}-H_{z_{m}-1}$$



                Letting ${lfloor x rfloor} to x-1,{lceil x rceil} to x+1 $ defines another function



                $$g_1(m) = H_{z_{m+1}-1}-H_{z_{m}+1-1}$$



                and we have the inequality



                $$g_1(m) lt g(m) lt g_0(m)$$



                Asymptotically this leads, up to $O(frac{1}{m^2})$, to the inequality



                $$frac{2}{m}- frac{1}{pi^2 m^2}< g(m) <frac{2}{m}+frac{1}{pi^2 m^2} $$



                This shows that $f_m$ goes to zero.



                ad (2)



                (to be continued)






                share|cite|improve this answer











                $endgroup$
















                  1












                  1








                  1





                  $begingroup$

                  This approach works in two steps and is generally applicable: first it transforms the sum to an alternating sum which then, in the second step, can be studied by the Dirichlet criterion.



                  Step 1: Transformation to an alternating sum



                  The partial sum in question is



                  $$s_n = sum_{k=1}^n c_ktag{1}$$



                  where



                  $$c_k = frac{cos(sqrt{k})}{k}tag{2}$$



                  Now collecting all subsequent summands with the same sign we can write



                  $$s_n = sum_{m=0}^M (-1)^m f_mtag{3}$$



                  where



                  $$f_0 = sum_{k=1}^{lfloor z_{1}rfloor} c_{k}tag{4a}$$



                  $$f_{mge 1} = (-1)^m sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} c_{k}tag{4b}$$



                  is the sum of terms between two adjacent roots $k=z_m$ and $k=z_{m+1}$ of $c(k) = 0$, and $M$ is some number depending on $n$ which can in principle be specified but it is normally not necessary as it goes to $infty$ together with $n$



                  Then, by an appropirate choice of the factor $(-1)^m$, all $f_m$ can be chosen to be positive quantities.



                  Step 2: Application of Dirichlet's criterion



                  Now we can apply the Dirichlet criterion to (3). This reads now as follows: $s_n$ is convergent if



                  (1) $f_m to 0$ for $mtoinfty$

                  (2) $f_m$ is monotonous



                  ad (1)



                  We have for $mge1$



                  $$|f_{m}| le g(m)$$



                  where we have dropped the $cos$ and have defined



                  $$g(m) = sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} frac{1}{k}
                  =H_{lfloor z_{m+1} rfloor}-H_{lceil z_{m}rceil-1}tag{5} $$



                  Here $H_n$ ist the harmonic number.



                  Now the zeroes of $c_{k}$ are given by



                  $$z_m = left(pi(m-frac{1}{2})right)^2tag{6}$$



                  Dropping Floor and Ceiling in $g(m)$ defines



                  $$g_0(m) = H_{z_{m+1}}-H_{z_{m}-1}$$



                  Letting ${lfloor x rfloor} to x-1,{lceil x rceil} to x+1 $ defines another function



                  $$g_1(m) = H_{z_{m+1}-1}-H_{z_{m}+1-1}$$



                  and we have the inequality



                  $$g_1(m) lt g(m) lt g_0(m)$$



                  Asymptotically this leads, up to $O(frac{1}{m^2})$, to the inequality



                  $$frac{2}{m}- frac{1}{pi^2 m^2}< g(m) <frac{2}{m}+frac{1}{pi^2 m^2} $$



                  This shows that $f_m$ goes to zero.



                  ad (2)



                  (to be continued)






                  share|cite|improve this answer











                  $endgroup$



                  This approach works in two steps and is generally applicable: first it transforms the sum to an alternating sum which then, in the second step, can be studied by the Dirichlet criterion.



                  Step 1: Transformation to an alternating sum



                  The partial sum in question is



                  $$s_n = sum_{k=1}^n c_ktag{1}$$



                  where



                  $$c_k = frac{cos(sqrt{k})}{k}tag{2}$$



                  Now collecting all subsequent summands with the same sign we can write



                  $$s_n = sum_{m=0}^M (-1)^m f_mtag{3}$$



                  where



                  $$f_0 = sum_{k=1}^{lfloor z_{1}rfloor} c_{k}tag{4a}$$



                  $$f_{mge 1} = (-1)^m sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} c_{k}tag{4b}$$



                  is the sum of terms between two adjacent roots $k=z_m$ and $k=z_{m+1}$ of $c(k) = 0$, and $M$ is some number depending on $n$ which can in principle be specified but it is normally not necessary as it goes to $infty$ together with $n$



                  Then, by an appropirate choice of the factor $(-1)^m$, all $f_m$ can be chosen to be positive quantities.



                  Step 2: Application of Dirichlet's criterion



                  Now we can apply the Dirichlet criterion to (3). This reads now as follows: $s_n$ is convergent if



                  (1) $f_m to 0$ for $mtoinfty$

                  (2) $f_m$ is monotonous



                  ad (1)



                  We have for $mge1$



                  $$|f_{m}| le g(m)$$



                  where we have dropped the $cos$ and have defined



                  $$g(m) = sum_{k={lceil z_{m}rceil}}^{lfloor z_{m+1} rfloor} frac{1}{k}
                  =H_{lfloor z_{m+1} rfloor}-H_{lceil z_{m}rceil-1}tag{5} $$



                  Here $H_n$ ist the harmonic number.



                  Now the zeroes of $c_{k}$ are given by



                  $$z_m = left(pi(m-frac{1}{2})right)^2tag{6}$$



                  Dropping Floor and Ceiling in $g(m)$ defines



                  $$g_0(m) = H_{z_{m+1}}-H_{z_{m}-1}$$



                  Letting ${lfloor x rfloor} to x-1,{lceil x rceil} to x+1 $ defines another function



                  $$g_1(m) = H_{z_{m+1}-1}-H_{z_{m}+1-1}$$



                  and we have the inequality



                  $$g_1(m) lt g(m) lt g_0(m)$$



                  Asymptotically this leads, up to $O(frac{1}{m^2})$, to the inequality



                  $$frac{2}{m}- frac{1}{pi^2 m^2}< g(m) <frac{2}{m}+frac{1}{pi^2 m^2} $$



                  This shows that $f_m$ goes to zero.



                  ad (2)



                  (to be continued)







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited Oct 25 '18 at 8:56

























                  answered Oct 24 '18 at 15:27









                  Dr. Wolfgang HintzeDr. Wolfgang Hintze

                  3,890621




                  3,890621






























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