- A$200(1-\ln 2) \,J$
- ✓$200(1-\ln 3 / 2) \,J$
- C$200(1+\ln 3 / 2) \,J$
- D$200 \,J$
Also, $Q=\int C d t$
For maximum work, efficiency should be maximum, i.e. for Carnot engine,
$\eta =1-\frac{T_{2}}{T_{1}}=1-\frac{200}{T}$
$\therefore \quad W =\int \eta Q_{\text {in }}$
$=-\int \limits_{600}^{400}\left(1-\frac{200}{T}\right) C d T$
$\Rightarrow \quad W =-C[T-200 \ln T]_{600}^{400}$
$=-C\left[-200+\ln \left(\frac{3}{2}\right) 200\right] J$
Here, $C=1$ (given)
$\therefore \quad W=200-200 \ln \left(\frac{3}{2}\right) \,J$
or $\quad W=200\left[1-\ln \left(\frac{3}{2}\right)\right] \,J$
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$y_1 =10 \sin \left(\omega t+\frac{\pi}{3}\right) cm$
$y_2 =5[\sin (\omega t)+\sqrt{3} \cos \omega t] \;cm$ respectively.
The amplitude of the resultant wave is $.............cm$.

