MCQ
A wheel of radius $R$ is trapped in a mud pit and spinning. As the wheel is spinning, it splashes mud blobs with initial speed $u$ from various points on its circumference. The maximum height from the centre of the wheel, to which a mud blob can reach is
  • A
    $u^{2} / 2 g$
  • $\frac{u^{2}}{2 g}+\frac{g R^{2}}{2 u^{2}}$
  • C
    $0$
  • D
    $R+\frac{u^{2}}{2 g}$

Answer

Correct option: B.
$\frac{u^{2}}{2 g}+\frac{g R^{2}}{2 u^{2}}$
b
$(b)$ Let a mud blob is detached from the circumference of wheel with initial speed $u$ at angle $\theta$ as shown below.

Height upto which mud blob can be thrown is

$h=$ Maximum height of projectile $+$ Height at which mud blob is thrown

$\therefore \quad h=\frac{u^{2} \sin ^{2} \theta}{2 g}+R \cos \theta \quad \dots(i)$

$h$ is maximum when $\frac{d h}{d \theta}=0$

$\Rightarrow \frac{d}{d \theta}\left(\frac{u^{2} \sin ^{2} \theta}{2 g}+R \cos \theta\right)$

$\Rightarrow \frac{u^{2}}{2 g} \cdot 2 \sin \theta \cos \theta-R \sin \theta=0$

$\Rightarrow \quad \frac{u^{2}}{g} \cdot \cos \theta=R \text { or } \cos \theta=\frac{R g}{u^{2}}$

$\Rightarrow \quad \sin ^{2} \theta=1-\frac{R^{2} g^{2}}{u^{2}}$

Substituting these values in Eq $(i)$, we get

$\lambda_{\max } =\frac{u^{2}}{2 g}\left(1-\frac{R^{2} g^{2}}{u^{4}}\right)+R\left(\frac{R g}{u^{2}}\right)$

$=\frac{u^{2}}{2 g}-\frac{R^{2} g}{2 u^{2}}+\frac{R^{2} g}{u^{2}}=\frac{u^{2}}{2 g}+\frac{R^{2} g}{2 u^{2}}$

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