The temperatures are defined as:
The efficiency of the Carnot engine (E) operating between $ T_H $ and $ T_C $ is calculated as:
$$ \eta_{12} = 1 - \frac{T_C}{T_H} = 1 - \frac{273}{473} = \frac{473 - 273}{473} = \frac{200}{473} $$
The efficiency of engine $ E_1 $ operating between $ T_H $ and $ T_M $ is:
$$ \eta_1 = 1 - \frac{T_M}{T_H} = 1 - \frac{373}{473} = \frac{473 - 373}{473} = \frac{100}{473} $$
The efficiency of engine $ E_2 $ operating between $ T_M $ and $ T_C $ is:
$$ \eta_2 = 1 - \frac{T_C}{T_M} = 1 - \frac{273}{373} = \frac{373 - 273}{373} = \frac{100}{373} $$
We compare $ \eta_{12} $ with $ \eta_1 + \eta_2 $ and $ \eta_1 \eta_2 $.
The sum of efficiencies $ \eta_1 + \eta_2 $ is:
$$ \eta_1 + \eta_2 = \frac{100}{473} + \frac{100}{373} = 100 \left( \frac{1}{473} + \frac{1}{373} \right)$$
$$= 100 \left( \frac{373 + 473}{473 \cdot 373} \right) = 100 \left( \frac{846}{473 \cdot 373} \right) = \frac{84600}{176329} \approx 0.4798 $$
The product of efficiencies $ \eta_1 \eta_2 $ is:
$$ \eta_1 \eta_2 = \frac{100}{473} \times \frac{100}{373} = \frac{10000}{176329} \approx 0.0567 $$
The efficiency $ \eta_{12} $ is:
$$ \eta_{12} = \frac{200}{473} \approx 0.4228 $$
Comparison Results:
We verify the relationship $ (1 - \eta_1)(1 - \eta_2) = 1 - \eta_{12} $:
$$ (1 - \eta_1)(1 - \eta_2) = \frac{373}{473} \times \frac{273}{373} = \frac{273}{473} $$
Since $ \frac{273}{473} = 1 - \frac{200}{473} $, it follows that:
$$ (1 - \eta_1)(1 - \eta_2) = 1 - \eta_{12} $$
Expanding this equation yields:
$$ 1 - \eta_1 - \eta_2 + \eta_1 \eta_2 = 1 - \eta_{12} $$
Rearranging the terms gives:
$$ \eta_{12} = \eta_1 + \eta_2 - \eta_1 \eta_2 $$
Given that $ \eta_1 \eta_2>0 $, it is confirmed that $ \eta_{12}<\eta_1 + \eta_2 $.
Conclusion:
The final result is $ \eta_{12}<\eta_1 + \eta_2 $.