Work, Power & Energy
Comprehension Passage: Comprehension - 16
Comprehension Passage: Comprehension - 17
Based on above information, answer the following questions.
The velocity given to the ball at point A so that it may hit the top of the building isComprehension Passage: Comprehension - 17
Based on above information, answer the following questions.
If the collision of ball with the building is elastic, then the angle with the horizontal at which the ball will rebound from the top of the building isComprehension Passage: Comprehension - 17
Based on above information, answer the following questions.
The horizontal distance of the ball from the foot of building where the ball strikes the horizontal ground isComprehension Passage: Comprehension - 18
The magnitude of the change in its velocity as it reaches a position, where the string is horizontalComprehension Passage: Comprehension - 18
When the particle's motion ceases to be circular, the angle made by the string with the horizontal isComprehension Passage: Comprehension - 18
When the particle leaves the circular path its velocity vector isComprehension Passage: Comprehension - 19
Comprehension Passage: Comprehension - 19
Comprehension Passage: Comprehension - 19
Comprehension Passage: Comprehension - 20
The normal force $N_{B}$ exerted by the track just after crossing point B isComprehension Passage: Comprehension - 20
The normal force $N_{C}$ at $C$ isComprehension Passage: Comprehension - 20
The distance travelled along the incline beyond point D where the block stops isComprehension Passage: Comprehension - 21
Net work done by the force $F$ on the block isComprehension Passage: Comprehension - 21
What is the final velocity of the block if initially it was at rest?Comprehension Passage: Comprehension - 21
Find the ratio of initial acceleration to final acceleration of the block.Comprehension Passage: Comprehension - 22
Comprehension Passage: Comprehension - 22
Comprehension Passage: Comprehension - 22
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Explanation:
$\mathrm{B} \rightarrow (\mathrm{s})$
$\mathrm{C} \rightarrow (\mathrm{r})$
(D) → (r)
Since $W_{total} = \Delta K$ and $W_{C} = -\Delta U$
and $W_{\mathrm{ext}} = \Delta U + \Delta K = (U_f + K_f) - (U_i + K_i)$

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Explanation:
$\mathrm{B} \rightarrow (\mathrm{r})$
$C \rightarrow (p)$
$\mathrm{D} \rightarrow (\mathrm{q})$
$v _ {B} ^ {2} = u _ {A} ^ {2} - 2 g h _ {A B} = (9 g \ell) - (2 g \ell) = 7 g \ell$
$\Rightarrow v _ {B} = \sqrt {7 g \ell}$
$\Rightarrow \frac {v _ {B} ^ {2}}{g ^ {\ell}} = 7$
Further, $T_{B}=\frac{mv_{B}^{2}}{\ell}=7mg$
$\Rightarrow \frac {T _ {B}}{2 m g} = \frac {7}{2}$
Again, $v_{C}^{2} = v_{A}^{2} - 2gh_{AC} = (9g\ell) - 2g(2\ell) = 5g\ell$
$\Rightarrow v _ {C} = \sqrt {5 g \ell}$
$\Rightarrow \frac {v _ {C} ^ {2}}{g ^ {\ell}} = 5$
Further, $T_{C} + mg = \frac{mv_{C}^{2}}{\ell}$
$\Rightarrow T _ {C} = 4 m g$
$\Rightarrow \frac {T _ {C}}{m g} = 4$

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Explanation:
$\mathrm{B} \rightarrow (\mathrm{p})$
$\mathrm{C} \rightarrow (\mathrm{s})$
$\mathrm{D} \rightarrow (\mathrm{q})$
$\mathrm{At} t = 4 \mathrm{s},$
$v = a t = 8 \mathrm{ms} ^ {- 1}$
and $s=\frac{1}{2}at^{2}=16m$
$K E = \frac {1}{2} m v ^ {2} = 3 2 \mathrm{J}$

From Work-Energy Theorem, we have
Work done by all the forces = $\Delta KE = 32$ J
Work done by gravity
$= - m g h = - (1) (1 0) (1 6) = - 1 6 0 \mathrm{J}$
Writing equation of motion, we have, $\sum F_y = ma$
$N \cos 3 0 ^ {\circ} + f \sin 3 0 ^ {\circ} - 1 0 = m a = 2$
$\Rightarrow \sqrt {3} \mathrm{N} + f = 2 4\tag{... (1}$
$\sum F _ {x} = 0$
$\Rightarrow \quad N \sin 3 0 ^ {\circ} = f \cos 3 0 ^ {\circ}$
$\Rightarrow N = \sqrt {3} f$
... (2)
Solving equations (1) and (2), we have
$f = 6 \mathrm{N}$
and $N = \frac{18}{\sqrt{3}} = 6\sqrt{3}\mathrm{N}$
So, $W_{N} = (N\cos \theta)(s) = (6\sqrt{3})\left(\frac{\sqrt{3}}{2}\right)(16) = 144 \mathrm{~J}$
and $W_{f} = (f\sin \theta)(s) = (6)\left(\frac{1}{2}\right)(16) = 48 \, \mathrm{J}$


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Explanation:
$\mathrm{B} \rightarrow (\mathrm{q})$
$C \rightarrow (p)$
$\mathrm{D} \rightarrow (\bar {t})$
$v _ {f} - v _ {i} = \mathrm{areaunder} a - x \mathrm{graph} = 1 2 \mathrm{ms} ^ {- 1}$
$\Rightarrow v _ {f} = 1 2 + 4 = 1 6 \mathrm{ms} ^ {- 1}$
$\Rightarrow \Delta K E = \frac {1}{2} m \left(v _ {f} ^ {2} - v _ {i} ^ {2}\right) = 1 2 0 \mathrm{J}$
Work done by all the forces = $\Delta KE = 120$ J
$K _ {f} = \frac {1}{2} m v _ {f} ^ {2} = 1 2 8 \mathrm{J}$
Work done by conservative forces = $U_{i} - U_{f} = 240$ J
Work done by external force i.e. $W_{ext}$ is given by
$W _ {\text {ext}} = \left( \begin{array}{c} \text {Total} \\ \text {work} \\ \text {done} \end{array} \right) - \left( \begin{array}{c} \text {Work done by} \\ \text {conservative} \\ \text {forces} \end{array} \right)$
$\Rightarrow W _ {\mathrm{ext}} = - 1 1 2 \mathrm{J}$

Column-I
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Explanation:
Angle between net force and the string can never be obtuse. It is $90^{\circ}$ at A, $0^{\circ}$ at B and acute in between.
Column-I
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Explanation:
B → (p, q, r)
C → (q, r)
D → (p, r)
Conceptual






