By Jaan Kalda (TalTech).
A thin long wire is made of a material that undergoes a phase transition so that its resistivity takes one of the two values, \rho_1 if its temperature is smaller than T_c, and \rho_2=2\rho_1 if the temperature is larger than T_c.
Assume the following:
(a) the heat flux per unit length of the wire to the ambient medium is W=\alpha (T-T_0), where \alpha is a constant, T denotes the temperature of the wire, and T_0 is the ambient temperature (T_0<T_c);
(b) the wire is so thin that the thermal flux along the wire can be almost everywhere neglected, and the characteristic thermalization time is much shorter than the time during which the voltage is changed;
(c) while the coefficient \alpha and cross-sectional area A are almost constant along the wire, due to imperfections, there are tiny variations;
(d) the length of the wire L\gg\sqrt A.
The voltage V applied to the ends of the wire is increased very slowly, at a constant rate (i.e. linearly in time), from zero until the whole wire has undergone a phase transition, and then reduced back to zero, at the same constant rate. Sketch how the total power P dissipated in the wire depends on time t.
Your sketch should show power and voltage values at any point where either P or its time derivative is discontinuous, expressed in terms of P_0=\alpha L(T_c-T_0) and V_0=L\sqrt{\alpha \rho_1(T_c-T_0)/A}. The solution is considered to be correct only if all these points have correct values, and all segments of the graph are qualitatively correct (e.g. a convex curve should not be drawn as a straight line).
Please submit the solution to this problem via e-mail to physcs.cup@gmail.com. The first intermediate results for Problem 2 will be published on 25th December, 13:00 GMT. The first hints will appear here on 1st January 2023, 13:00 GMT. After the publication of the first hint, the base score is reduced to 0.9 pts. For full regulations, see the “Participate” tab.