Only One Metre

Calculus Level 5

Suppose there exists a string that is wrapped snugly around the Earth at its equator. You add one metre to the string and hold it up at a point until all the slack is gone. Find the height between the point at which the string is being held up at and the ground directly below the string.


  • Assume the Earth is perfectly spherical and has a radius of 6400km

  • Assume that the string does not stretch

  • Answer in metres to one decimal place

  • Note that the question says that the string is being lifted at one point , not that it is being lifted evenly throughout the planet (basically, the string is not concentric to the equator after 1 metre is added.)


The answer is 121.6.

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1 solution

Sharky Kesa
Apr 2, 2016

Since people are misinterpreting the question, I will write a solution to show where they are going wrong.

Note that the string is tangent to the Earth from where it is being held to the point of first contact with the surface. These are the two tangents from the point to the Earth as a result. Let's call the lengths of these tangents a a . Let's call the height of the point from the ground h h and the radius of the Earth r r (we will substitute r = 6400000 m r=6400000 \mathrm{m} later).

Consider a line joining the point to the centre of the Earth. This has a length of r + h r+h , which is equal to a 2 + r 2 \sqrt{a^2+r^2} by Pythagoras Theorem. Call the angle subtended by the line connecting the centre of the Earth to the point of tangency of the string and the line connecting the point to the centre of the earth as θ \theta (in radians).

The length of the string not in contact with the Earth is 2 a 2a . Also, the length of the corresponding circular arc is 2 r θ 2r\theta . Thus, we have

2 a = 2 r θ + 1 a = r θ + 1 2 a r = θ + 1 2 r tan θ = θ + 1 2 r \begin{aligned} 2a &= 2r\theta + 1\\ a &= r\theta + \dfrac {1}{2}\\ \dfrac {a}{r} &= \theta + \dfrac {1}{2r}\\ \tan \theta &= \theta + \dfrac {1}{2r} \end{aligned}

The Maclaurin series for tan θ \tan \theta is θ + θ 3 3 + \theta+\dfrac{\theta^3}{3} + \ldots . Hence,

θ + θ 3 3 θ + 1 2 r θ 3 3 12800000 θ 15 3 400 \begin{aligned} \theta+\dfrac {\theta^3}{3} &\approx \theta + \dfrac {1}{2r}\\ \theta^3 &\approx \dfrac {3}{12800000}\\ \theta &\approx \dfrac {\sqrt[3]{15}}{400} \end{aligned}

From this, we get the value of a a is

a = 6400000 × 15 3 400 + 1 2 = 16000 15 3 + 1 2 \begin{aligned} a &= 6400000 \times \dfrac {\sqrt[3]{15}}{400} + \dfrac {1}{2}\\ &= 16000 \sqrt[3]{15} + \dfrac {1}{2} \end{aligned}

From this we get the value of r + h r+h as

r + h = ( 16000 15 3 + 1 2 ) 2 + 6400000 0 2 6400121.6 m h 121.6 m \begin{aligned} r+h &= \sqrt{\left (16000 \sqrt[3]{15} + \dfrac {1}{2}\right )^2 + 64000000^2}\\ &\approx 6400121.6 \mathrm{m}\\ h &\approx 121.6 \mathrm{m} \end{aligned}

Thus, the height is 121.6 m 121.6 \mathrm{m} .

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