Physics, asked by venkateshmadichetti, 10 months ago

a stone of mass m is held at rest in water.The stone is released and falls vertically a distance h.the stone reaches a speed v.Which expression gives the work done against resistive force ?

Answers

Answered by nirman95
86

Answer:

Given: Mass of stone = m

distance covered = h

velocity reached = v

To find : work done against Frictional force

Concept: In this case, the net Frictional force is provided by 2 forces namely

a) Buoyant force

b) Stroke's force

Calculation: Let the acceleration offered by Frictional force be "a"

Now applying equation of kinematics:

v² = u² + 2as

=> v² = 0² + 2×a×h

=> v² = 2ah

=> a = (v²/2h)

Now force experienced

= mass × acceleration

= m×a

= m (v²/2h)

Now work done = force ×displacement

W = m(v²/2h)× h

W = (mv²/2)

So the answer is [mv²/2].

Answered by Sharad001
190

Question :-

a stone of mass m is held at rest in water.The stone is released and falls vertically a distance h.the stone reaches a speed v.Which expression gives the work done against resistive force ?

Answer:-

\boxed{\sf{work \:  =  \frac{1}{2}m \:  {v}^{2}  }} \:

To Find :-

→ Find work done against Force .

Formula used :-

Here we used,

 \sf{ third \: equation \: of \: motion} \\  \\ \rightarrow \: \boxed{ \sf{  {v}^{2}  =  {u}^{2}  + 2as}} \\  \\ \rightarrow \small \sf{  \boxed{\sf{work \:  = force \:  \times  \: displacement}}} \\  \\ \rightarrow \small \sf{ \boxed{\sf{ force \:  =  \: mass \:  \times \: acceleration}}}

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Step - by - step explanation :-

Let, acceleration is "a",

Initial velocity ( u ) = 0,

Displacement is "h",

Now applying the third equation of motion ,

\rightarrow \:  \sf{ {v}^{2}  = 0 + 2a \times h }\:  \\  \\ \rightarrow \:  \sf{a \:  =  \frac{ {v}^{2} }{2h} } \:  \:  \: ......(1)

Now find force to finding the work done ,

\rightarrow \:  \sf{force \:  = m \:  \times a }\\  \\ \rightarrow \: \sf{ force \:  = m \:  \times  \frac{ {v}^{2} }{2h} } \:  \:  \: ....(2) \\  \\

Now required work done is ,

  \boxed{ \sf{work \:  = force \:  \times displacement \: }} \\  \\ \bf{ from \: (2)} \\  \\ \rightarrow \:  \sf{work \:  = m \:  \frac{ {v}^{2} }{2h}  \times h} \\  \\ \rightarrow \:   \boxed{\sf{work \:  =  \frac{1}{2}m \:  {v}^{2}  }}

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