- A$\frac{4 \alpha \beta}{(\alpha+\beta)} t ^{2}$
- B$\frac{2 \alpha \beta}{(\alpha+\beta)} t ^{2}$
- ✓$\frac{\alpha \beta}{2(\alpha+\beta)} t ^{2}$
- D$\frac{\alpha \beta}{4(\alpha+\beta)} t ^{2}$
$t _{1}+ t _{2}= t$
$v _{0}\left(\frac{1}{\alpha}+\frac{1}{\beta}\right)= t$
$\Rightarrow v _{0}=\frac{\alpha \beta t }{\alpha+\beta}$
Distance $=$ area of $v - t$ graph
$=\frac{1}{2} \times t \times v _{0}=\frac{1}{2} \times t \times \frac{\alpha \beta t }{\alpha+\beta}=\frac{\alpha \beta t ^{2}}{2(\alpha+\beta)}$
Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.
$\sqrt{6}$ times faster.
$\sqrt{6}$ times slower.
The change in internal energy of the gas during the transition is ............$\;kJ$


$(A)$ $v_0^2-2 g h=\frac{1}{2} g R$
$(B)$ $v_0^2-2 g h=\frac{\sqrt{3}}{2} g R$
$(C)$ the centripetal force required at points $x$ and $z$ is zero
$(D)$ the centripetal force required is maximum at points $x$ and $z$
