IPhO 1971, Теория и експеримент — Задача 3. Question 3.
V International Physics Olympiad, 1971. Sofia, Bulgaria
Внимание: Бележка към темата
Решенията са архивна адаптация на Victor Ivanov, както е посочено в оригинала. Формули (1.13), (1.17) и (4.6), както и повтореното означение P₂ в числените резултати на задача 2, са запазени според източника. Добавеният множител g в краткия отговор на задача 1 е отделно обозначена редакционна поправка; текстът на архивното решение остава непроменен.
Source
The problems and the solutions are adapted by Victor Ivanov University of Sofia, Faculty of Physics, 5 James Bourchier Blvd., 1164 Sofia, Bulgaria
Reference: O. F. Kabardin, V. A. Orlov, in “International Physics Olympiads for High School Students”, eds. V. G. Razumovski, Moscow, Nauka, 1985. (In Russian).
Theoretical problems
Solutions — source
Solutions to the problems of the 5-th International Physics Olympiad, 1971, Sofia, Bulgaria
The problems and the solutions are adapted by Victor Ivanov Sofia State University, Faculty of Physics, 5 James Bourcier Blvd., 1164 Sofia, Bulgaria
Reference: O. F. Kabardin, V. A. Orlov, in “International Physics Olympiads for High School Students”, eds. V. G. Razumovski, Moscow, Nauka, 1985. (In Russian).
Theoretical problems
Условие
Four batteries of EMF , , , and , four capacitors with the same capacitance , and four equivalent resistors are connected in the circuit shown in Fig. 3. The internal resistance of the batteries is negligible.
• Calculate the total energy accumulated on the capacitors when a steady state of the system is established.
• The points H and B are short connected. Find the charge on the capacitor in the new steady state.

Отговори
- • 26 μJ
- • 0 C
Решение
A circuit equivalent to the given one is shown in Fig. 3. In a steady state (the capacitors are completely charged already) the same current flows through all the resistors in the closed circuit ABFGHDA. From the Kirchhoff’s second rule we obtain:
(3.1)
Next we apply this rule for the circuit ABCDA:
(3.2) ,
where is the potential difference across the capacitor . By using the expression (3.1) for , and the equation (3.2) we obtain:
(3.3)
Similarly, we obtain the potential differences and across the capacitors and by considering circuits BFGCB and FGHEF:
(3.4)
(3.5)
Finally, the voltage across is found by applying the Kirchhoff’s rule for the outermost circuit EHDAH:
(3.6)
The total energy of the capacitors is expressed by the formula:
(3.7)

When points B and H are short connected the same electric current flows through the resistors in the BFGH circuit. It can be calculated, again by means of the Kirchhoff’s rule, that:
(3.8)
The new steady-state voltage on is found by considering the BFGCB circuit:
(3.9)
or finally:
(3.10)
Therefore the charge on in the new steady state is zero.
Оригинал в Архива: ipho71_problems.pdf · решение от архива: ipho71_solutions.pdf · допълнителни данни: 1971_Sofia_Problems.pdf · допълнителни данни: 1971_Sofia_Solutions.pdf