IPhO 1982, Теория и експеримент — Задача 3. Hot-air-balloon

Problems of the 13th International Physics Olympiad (Malente, 1982) · 10 т.

Abstract

The 13th International Physics Olympiad took place in 1982 in the Federal Republic of Germany. This article contains the competition problems, their solutions and a grading scheme.

Увод

In 1982 the Federal Republic of Germany was the first host of the Physics Olympiad outside the so-called Eastern bloc. The 13th International Physics Olympiad took place in Malente, Schleswig-Holstein. The competition was funded by the German Federal Ministry of Science and Education. The organisational guidelines were laid down by the work group “Olympiads for pupils” of the conference of ministers of education of the German federal states. The Institute for Science Education (IPN) at the University of Kiel was responsible for the realisation of the event. A commission of professors, whose chairman was appointed by the German Physical Society, were concerned with the formulation of the competition problems. All other members of the commission came from physics department of the university of Kiel or from the college of education at Kiel.

The problems as usual covered different fields of classical physics. In 1982 the pupils had to deal with three theoretical and two experimental problems, whereas at the previous Olympiads only one experimental task was given. However, it seemed to be reasonable to put more stress on experimental work. The degree of difficulty was well balanced. One of the theoretical problems could be considered as quite simple (problem 3: “hot-air balloon”). Another theoretical problem (problem 1: “fluorescent lamp”) had a mean degree of difficulty and the distribution of the points was a normal distribution with only a few excellent and only a few unsatisfying solutions. The third problem (problem 2: “oscillation coat hanger”) turned out to be the most difficult problem. This problem was generally considered as quite interesting because different ways of solving were possible. About one third of the pupils did not find an adequate start to the problem, but nearly one third of the pupils was able to solve the substantial part of the problem. That means, this problem polarized between the pupils. The two experimental tasks were quite different in respect of the input for the experimental setup and the time required for dealing with the problems, whereas they were quite similar in the degree of difficulty. Both required demandingly theoretical considerations and experimental skills. Both experimental problems turned out to be rather difficult. The tasks were composed in a way that on the one hand almost every pupil had the possibility to come to certain partial results and that there were some difficulties on the other hand which could only be solved by very few pupils. The difficulty in the second experimental problem (problem5: “motion of a rolling cylinder”) was the explanation of the experimental results, which were initially quite surprising. The difficulty in the other task (problem 4: “lens experiment") was the revealing of an observation method with a high accuracy (parallax). The five hours provided for solving the two experimental problems were slightly too short. According to that, in both experiments only a few pupils came up with excellent solutions. In problem 5 nobody got the full points.

The problems presented here are based on the original German and English versions of the competition problems. The solutions are complete but in some parts condensed to the essentials. Almost all of the original hand-made figures are published here.

Contact: Leibniz-Institute for Science Education (IPN) at the University of Kiel, Olshausenstrasse 62, 24098 Kiel, Germany, ipho@ipn.uni-kiel.de

Условие

Consider a hot-air balloon with fixed volume VB=1.1 m3V_B = 1.1\ \mathrm{m^3}. The mass of the balloon-envelope, whose volume is to be neglected in comparison to VBV_B, is mH=0.187 kgm_H = 0.187\ \mathrm{kg}.

The balloon shall be started, where the external air temperature is ϑ1=20 ∘C\vartheta_1 = 20\ {}^{\circ}\mathrm{C} and the normal external air pressure is po=1.013⋅105 Pap_o = 1.013 \cdot 10^5\ \mathrm{Pa}. Under these conditions the density of air is ρ1=1.2 kg/m3\rho_1 = 1.2\ \mathrm{kg/m^3}.

a) What temperature ϑ2\vartheta_2 must the warmed air inside the balloon have to make the balloon just float? [3 т.]

b) First the balloon is held fast to the ground and the internal air is heated to a steady-state temperature of ϑ3=110 ∘C\vartheta_3 = 110\ {}^{\circ}\mathrm{C}. The balloon is fastened with a rope.

Calculate the force on the rope. [2 т.]

c) Consider the balloon being tied up at the bottom (the density of the internal air stays constant). With a steady-state temperature ϑ3=110 ∘C\vartheta_3 = 110\ {}^{\circ}\mathrm{C} of the internal air the balloon rises in an isothermal atmosphere of 20 ∘C20\ {}^{\circ}\mathrm{C} and a ground pressure of p0=1.013⋅105 Pap_0 = 1.013 \cdot 10^5\ \mathrm{Pa}. Which height hh can be gained by the balloon under these conditions? [3 т.]

d) At the height hh the balloon (question c)) is pulled out of its equilibrium position by 10 m and then is released again.

Find out by qualitative reasoning what kind of motion it is going to perform! [2 т.]

Отговори

Решение


Оригинал в Архива: ipho82.pdf