IPhO 2010, Експеримент — Задача 1. Elasticity of sheets

41st International Physics Olympiad, Croatia – Experimental Competition, July 21st, 2010 — Experimental problem 1 · 21 юли 2010 г. · 10 т.

Условие

There are two experimental problems. The setup on your table is used for both problems. You have 5 hours to complete the entire task (1&2).

Experimental problem 1: Elasticity of sheets

Introduction

Springs are objects made from elastic materials which can be used to store mechanical energy. The most famous helical springs are well described in terms of Hooke’s law, which states that the force with which the spring pushes back is linearly proportional to the distance from its equilibrium length: F=−kΔxF = -k\Delta x, where kk is the spring constant, Δx\Delta x is the displacement from equilibrium, and FF is the force [see Fig. 1(a)]. However, elastic springs can have quite different shapes from the usual helical springs, and for larger deformations Hooke’s law does not generally apply. In this problem we measure the properties of a spring made from a sheet of elastic material, which is schematically illustrated in Fig. 1(b).

Two panels. (a) A mass m rests on a plate supported by a helical spring inside a container. (b) A mass m rests on a plate that compresses a rolled elastic sheet into a stadium shape with two semicircular ends of radius R0; the height of the compressed sheet is marked 2R0.
Figure 1. Illustrations of (a) a helical spring and (b) a spring made from a sheet of elastic material rolled up into a cylinder. When the latter spring is sufficiently compressed, its shape can be approximated as a stadium with two semicircles of radii R0R_0 (see text).

Transparent foil rolled into a cylindrical spring

Suppose that we take a sheet of elastic material (e.g. a transparent foil) and bend it. The more we bend it, the more elastic energy is stored in the sheet. The elastic energy depends on the curvature of the sheet. Parts of the sheet with larger curvature store more energy (flat parts of the sheet do not store energy because their curvature is zero). The springs used in this experiment are made from rectangular transparent foils rolled into cylinders (see Fig. 2). The elastic energy stored in a cylinder is

Eel=κ21Rc2A,(1)E_{el} = \frac{\kappa}{2}\frac{1}{R_c^2}A, \qquad (1)

where AA denotes the area of the cylinder's side (excluding its bases), RcR_c denotes its radius, and the parameter κ\kappa, referred to as the bending rigidity, is determined by the elastic properties of the material and the thickness of the sheet. Here we neglect the stretching of the sheets.

A cylinder drawn obliquely; its length is marked l along a dashed line and the radius of its end face is marked Rc.
Figure 2. A schematic picture of an elastic sheet rolled into a cylinder of radius RcR_c and length ll.

Suppose that such a cylinder is compressed as in Fig. 1(b). For a given force applied by the press (FF), the displacement from equilibrium depends on the elasticity of the transparent foil. For some interval of compression forces, the shape of the compressed transparency foil can be approximated with the shape of a stadium, which has a cross section with two straight lines and two semicircles, both of radius R0R_0. It can be shown that the energy of the compressed system is minimal when

R02=lκπ2F.(2)R_0^2 = \frac{l\kappa\pi}{2F}. \qquad (2)

The force is measured by the scale calibrated to measure mass mm, so F=mgF = mg, g=9.81 m/s2g = 9.81\ \mathrm{m/s^2}.

Experimental setup (1st problem)

The following items (to be used for the 1st problem) are on your desk:

  1. Press (together with a stone block); see separate instructions if needed
  2. Scale (measures mass up to 5000 g, it has TARA function, see separate instructions if needed)
  3. Transparency foils (all foils are 21 cm x 29.7 cm, the blue foil is 200 µm thick, and the colorless foil is 150 µm thick); please, do ask for the extra foils if you need them.
  4. Adhesive (scotch) tape
  5. Scissors
  6. Ruler with a scale
  7. A rectangular wooden plate (the plate is to be placed on a scale, and the foil sits on the plate)

The setup is to be used as in Fig. 3. The upper plate of the press can be moved downward and upward using a wing nut, and the force (mass) applied by the press is measured with the scale. Important: The wing nut moves 2 mm when rotated 360 degrees. (Small aluminum rod is not used in Experiment 1.)

Photo of the press: a lower and an upper plywood plate joined by a vertical grey bar with a threaded rod and wing nut; a stone block sits on the upper plate, and a blue foil cylinder is compressed between the upper plate and a wooden plate lying on a digital scale.
Figure 3. The photo of a setup for measuring the bending rigidity.

Tasks

  1. Roll the blue foils into cylinders, one along the longer side, and the other along its shorter side; use the adhesive tape to fix them. The overlap of the sheet should be about 0.5 cm.

1. (a) Measure the dependence of the mass read by the scale on the separation between the plates of the press for each of the two cylinders. (1.9 points)

1. (b) Plot your measurements on appropriate graphs. Using the ruler and eye as the guide, draw lines through the points and determine the bending rigidities κ\kappa for the cylinders. Mark the region where the approximate relation (the stadium approximation) holds. Estimate the value of R0Rc\dfrac{R_0}{R_c} below which the stadium approximation holds; here RcR_c is the radius of the non-laden cylinder(s). (4.3 points)

The error analysis of the results is not required.

2. Measure the bending rigidity of a single colorless transparent foil. (2.8 points)

3. The bending rigidity κ\kappa depends on the Young’s modulus YY of elasticity of the isotropic material, and the thickness dd of the transparent foil according to

κ=Yd312(1−ν2),(3)\kappa = \frac{Yd^3}{12(1-\nu^2)}, \qquad (3)

where ν\nu is the Poisson ratio for the material; for most materials ν≈1/3\nu \approx 1/3. From the previous measurements, determine the Young’s modulus of the blue and the colorless transparent foil. (1.0 points)

Отговори

Решение


Оригинал в Архива: exp1.pdf · официални решения: exp1_sol.pdf