Does the length be useful everytime !!!!

A rubber string of mass m m and rigidity k k is suspended at one end. Determine the elongation of the string.

Assumptions

  • m = 1 kg m = 1 \mbox{ kg}
  • k = 500 N/m k = 500 \mbox{ N/m}
  • g = 10 m/s 2 g = 10 \mbox{ m/s}^2


The answer is 0.01.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

1 solution

A K
Apr 28, 2014

The extension of a spring is given by F k = Δ x \frac{F}{k} = \Delta x where F = m g F = mg .

Therefore, m g k = Δ x \frac{mg}{k} = \Delta x .

The weight acting on a particular point along the string can be given by m g n mgn where n n = how far up the string the point is, expressed as a fraction. Therefore, 0 n 1 0\leq n \leq 1 .

0 is at the bottom of the string (no weight/force acts to extend it) and 1 is at the top of the string where the string's entire weight provides a force to extend it.

We want the extension of the whole string, so we can integrate the function between 0 and 1, because this interval for n n encompasses the string's whole length.

0 1 m g n k d n = m g n 2 2 k 0 1 = m g 2 k = 1 × 10 2 × 500 = 0.01 m \int_0^1 \frac{mgn}{k}\;\mathrm{d}n= \tfrac{mgn^{2}}{2k} \Big|_0^1 = \frac{mg}{2k} = \frac{1 \times 10}{2 \times 500} = \boxed{0.01m} .

I guess you could also just state that the 'average' weight (force) acting on the whole string is m g 2 \frac{mg}{2} , i.e. half the total weight, and substitute this directly into the force-extension equation to yield the same answer.

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...