Going Around In A Discrete Harmonic Spiral

Calculus Level 5

A man is standing at the origin. First, he walks 1 1 unit in the positive x x direction and reaches ( 1 , 0 ) (1,0) . Then, he turns 6 0 o 60^o counterclockwise and walks 1 / 2 1/2 units. Again, he turns 6 0 o 60^o counterclockwise and walks 1 / 3 1/3 units. He continues this endlessly.

Find the distance between his initial and final position.


The answer is 1.047.

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3 solutions

Pratik Shastri
Jan 2, 2015

Let the unit vector along the + x +x direction be i ^ \hat{i} and that along the + y +y direction be j ^ \hat{j} . Let O O be the origin.

The position vector of the final position (say P P ) wrt O O of the man is given by the vector sum of all the displacements, IE

O P = i ^ + 1 2 ( cos π 3 i ^ + sin π 3 j ^ ) + 1 3 ( cos 2 π 3 i ^ + sin 2 π 3 j ^ ) + = ( 1 + 1 2 cos π 3 + 1 3 cos 2 π 3 + ) i ^ + ( 1 2 sin π 3 + 1 3 sin 2 π 3 + ) j ^ = ( n = 1 1 n cos ( n 1 ) π 3 ) S 1 i ^ + ( n = 1 1 n sin ( n 1 ) π 3 ) S 2 j ^ = S 1 i ^ + S 2 j ^ \begin{aligned} \vec{OP}&=\hat{i}+\dfrac{1}{2}\left(\cos{\dfrac{\pi}{3}}\hat{i}+\sin{\dfrac{\pi}{3}}\hat{j}\right)+\dfrac{1}{3}\left(\cos{\dfrac{2\pi}{3}}\hat{i}+\sin{\dfrac{2\pi}{3}}\hat{j}\right)+\cdots\\ &=\left(1+\dfrac{1}{2}\cos{\dfrac{\pi}{3}}+\dfrac{1}{3}\cos{\dfrac{2\pi}{3}}+\cdots\right)\hat{i}+\left(\dfrac{1}{2}\sin{\dfrac{\pi}{3}}+\dfrac{1}{3}\sin{\dfrac{2\pi}{3}}+\cdots\right)\hat{j}\\&=\underbrace{\left(\sum_{n=1}^{\infty} \dfrac{1}{n}\cos {\dfrac{(n-1)\pi}{3}}\right)}_{S_1}\hat{i}+\underbrace{\left(\sum_{n=1}^{\infty} \dfrac{1}{n}\sin {\dfrac{(n-1)\pi}{3}}\right)}_{S_2}\hat{j}\\ &=S_1 \hat{i}+S_2 \hat{j}\end{aligned}

Clearly, S 1 = n = 1 e i ( n 1 ) π / 3 n S_1=\Re \displaystyle\sum_{n=1}^{\infty}\dfrac{e^{i(n-1)\pi/3}}{n} and S 2 = n = 1 e i ( n 1 ) π / 3 n S_2=\Im \displaystyle\sum_{n=1}^{\infty}\dfrac{e^{i(n-1)\pi/3}}{n}

Let us evaluate S = n = 1 e i ( n 1 ) π / 3 n S=\displaystyle\sum_{n=1}^{\infty}\dfrac{e^{i(n-1)\pi/3}}{n} .

For that, consider the Maclaurin expansion of ( 1 x ) 1 (1-x)^{-1} . ( 1 x ) 1 = n = 0 x n (1-x)^{-1}=\sum_{n=0}^{\infty} x^n Integrate on LHS and RHS, note that the constant of integration is 0 0 , and then divide by x x to obtain n = 0 x n n + 1 = n = 1 x n 1 n = log ( 1 x ) x ( 1 ) \sum_{n=0}^{\infty} \dfrac{x^n}{n+1}=\sum_{n=1}^{\infty} \dfrac{x^{n-1}}{n}=-\dfrac{\log(1-x)}{x} \ \ \ \ \ \ \ \ \ \ \ \ (1) Therefore from ( 1 ) (1) , S = log ( 1 e i π / 3 ) e i π / 3 = π 2 3 + i π 6 S=-\dfrac{\log(1-e^{i\pi/3})}{e^{i\pi/3}}=\dfrac{\pi}{2\sqrt{3}}+i\dfrac{\pi}{6}

Hence, O P = { S } i ^ + { S } j ^ = π 2 3 i ^ + π 6 j ^ \vec{OP}=\Re\{S\}\hat{i}+\Im\{S\}\hat{j}=\dfrac{\pi}{2\sqrt{3}}\hat{i}+\dfrac{\pi}{6}\hat{j}

So, finally, O P = π 3 1.047 |\vec{OP}|=\dfrac{\pi}{3}\approx \boxed{\color{#3D99F6}{1.047}}

Or we could have done it by the use of complex numbers. the sum would be: d = r = 0 e i π r / 3 r + 1 = π 2 3 + i π 6 1.047 d=\left| \sum _{ r=0 }^{ \infty }{ \frac { { e }^{ i\pi r/3 } }{ r+1 } } \right| =\left| \frac { \pi }{ 2\sqrt { 3 } } +i\frac { \pi }{ 6 } \right| \approx 1.047 But even after solving it I entered , eventually the wrong answer due to calculation errors!!

Kunal Gupta - 6 years, 5 months ago

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It's essentially the same thing.

Pratik Shastri - 6 years, 5 months ago

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The problem with the man is that he had to walk infinite distance.

Krishna Sharma - 6 years, 5 months ago

I used the same logic. I am attaching a graphic to show how the spiral looks like.

Nice! How did you generate the graphic?

Pratik Shastri - 6 years, 5 months ago

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I just used a Microsoft Excel spreadsheet. It is easy.

Chew-Seong Cheong - 6 years, 5 months ago
Joe Mansley
Jun 18, 2020

k = 1 e ( k 1 ) π i / 3 k = e π i / 3 ln ( 1 e π i / 3 ) = e π i / 3 ln ( 1 / 2 i ( 3 ) / 2 ) = e π i / 3 ln e π i / 3 = e π i / 3 ( π i / 3 ) \sum_{k=1}^\infty \frac{e^{(k-1)\pi i/3}}{k} = -e^{-\pi i/3} \ln{(1-e^{\pi i/3})} = -e^{-\pi i/3} \ln{(1/2 -i\sqrt(3)/2)} = -e^{-\pi i/3} \ln{e^{-\pi i/3}} = -e^{-\pi i/3} (-\pi i/3)

Which has modulus π 3 \frac{\pi}{3} .

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