1 unit in the positive x direction and reaches ( 1 , 0 ) . Then, he turns 6 0 o counterclockwise and walks 1 / 2 units. Again, he turns 6 0 o counterclockwise and walks 1 / 3 units. He continues this endlessly.
A man is standing at the origin. First, he walksFind the distance between his initial and final position.
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Or we could have done it by the use of complex numbers. the sum would be: d = ∣ ∣ ∣ ∑ r = 0 ∞ r + 1 e i π r / 3 ∣ ∣ ∣ = ∣ ∣ ∣ 2 3 π + i 6 π ∣ ∣ ∣ ≈ 1 . 0 4 7 But even after solving it I entered , eventually the wrong answer due to calculation errors!!
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It's essentially the same thing.
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The problem with the man is that he had to walk infinite distance.
I used the same logic. I am attaching a graphic to show how the spiral looks like.
Nice! How did you generate the graphic?
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I just used a Microsoft Excel spreadsheet. It is easy.
∑ k = 1 ∞ k e ( k − 1 ) π i / 3 = − 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 )
Which has modulus 3 π .
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Let the unit vector along the + x direction be i ^ and that along the + y direction be j ^ . Let O be the origin.
The position vector of the final position (say P ) wrt O of the man is given by the vector sum of all the displacements, IE
O P = i ^ + 2 1 ( cos 3 π i ^ + sin 3 π j ^ ) + 3 1 ( cos 3 2 π i ^ + sin 3 2 π j ^ ) + ⋯ = ( 1 + 2 1 cos 3 π + 3 1 cos 3 2 π + ⋯ ) i ^ + ( 2 1 sin 3 π + 3 1 sin 3 2 π + ⋯ ) j ^ = S 1 ( n = 1 ∑ ∞ n 1 cos 3 ( n − 1 ) π ) i ^ + S 2 ( n = 1 ∑ ∞ n 1 sin 3 ( n − 1 ) π ) j ^ = S 1 i ^ + S 2 j ^
Clearly, S 1 = ℜ n = 1 ∑ ∞ n e i ( n − 1 ) π / 3 and S 2 = ℑ n = 1 ∑ ∞ n e i ( n − 1 ) π / 3
Let us evaluate S = n = 1 ∑ ∞ n e i ( n − 1 ) π / 3 .
For that, consider the Maclaurin expansion of ( 1 − x ) − 1 . ( 1 − x ) − 1 = n = 0 ∑ ∞ x n Integrate on LHS and RHS, note that the constant of integration is 0 , and then divide by x to obtain n = 0 ∑ ∞ n + 1 x n = n = 1 ∑ ∞ n x n − 1 = − x lo g ( 1 − x ) ( 1 ) Therefore from ( 1 ) , S = − e i π / 3 lo g ( 1 − e i π / 3 ) = 2 3 π + i 6 π
Hence, O P = ℜ { S } i ^ + ℑ { S } j ^ = 2 3 π i ^ + 6 π j ^
So, finally, ∣ O P ∣ = 3 π ≈ 1 . 0 4 7