| 1 $T_{H}^{\prime}=T_{C}^{\prime}=\dfrac{T_{H}+T_{C}}{2}$ | 0.30 |
|
| 1 $r_{\max }=\dfrac{\delta-\eta_{0}}{2 \delta}$ | 1.20 |
|
| 2 $12.5 \%$ | 0.40 |
|
| 1 $\eta_{e}=\dfrac{7 \delta \eta_{0}}{4\left(\delta+\eta_{0}\right)}$ | 1.00 |
|
| 2 $21 \%$ | 0.30 |
|
| 1 $V \cdot T^{-2}=\operatorname{const}$ или эквивалентное | 0.80 |
|
| 1 $U(V, T)=\dfrac{\alpha T^{4}}{4 V}$ или эквивалентное | 1.20 |
|
| 1 Получено уравнение, эквивалентное $2 x \dfrac{\mathrm d f}{\mathrm d x}-f=-\dfrac{\alpha}{4} x^{2}$ | 1.60 |
|
| 2 $p(V, T)=-\dfrac{\alpha T^{4}}{12 V^{2}}$ или эквивалентное | 0.80 |
|
| 1 $U(p, V)=-3 p V$ | 0.30 |
|
| 2 $p V^{2 / 3}=\operatorname{const}$ | 0.30 |
|
| $473 \%$ | ||
| 2 $472 \%~\ldots~474 \%$ | 1.20 |
|
| 3 $470 \%~\ldots~475 \%$ | 0.30 |
|
| 1 $21.5 \%$ | 0.60 |
|