Work Power & Energy

NEET Physics · 97 questions · Page 10 of 10 · Click an option or "Show Solution" to reveal answer

Q91
A ball of mass 0.20.2 kgkg is thrown vertically upwards by applying a force by hand. If the hand moves 0.20.2 mm while applying the force and the ball goes upto 22 mm height further, find the magnitude of the force. (consider g=10m/s2g = 10\,m/{s^2}).
A 4N4N
B 1616 NN
C 2020 NN
D 2222 NN
Correct Answer
Option D
Solution

According to energy conservation law, Work done by the hand and due to gravity = total change in the kinetic energy Initially the the ball is at rest and finally at top its velocity become zero so total change in kinetic energy

ΔK\Delta K

= 0

Whand+Wgravity=ΔK{W_{hand}} + {W_{gravity}} = \Delta K

[Here distance covered would be 0.2 meter for force by hand as force is applied while ball is in contact with hand.

And gravity will still work while ball is in contact with hand so total distance due to gravity would be 2 + 0.2 = 2.2 meter.]

F(0.2)(0.2)(10)(2.2)\Rightarrow F\left( {0.2} \right) - \left( {0.2} \right)\left( {10} \right)\left( {2.2} \right)
=0F=22N= 0 \Rightarrow F = 22\,N

\therefore Option (D) is correct.

Q92
A force F=2i^+bj^+k^\overrightarrow{\mathrm{F}}=2 \hat{i}+\mathrm{b} \hat{j}+\hat{k} is applied on a particle and it undergoes a displacement i^2j^k^\hat{i}-2 \hat{j}-\hat{k} What will be the value of bb, if work done on the particle is zero.
A 13\dfrac{1}{3}
B 12\dfrac{1}{2}
C 0
D 2
Correct Answer
Option B
Solution

To determine the value of

bb

such that the work done on the particle is zero, follow these steps: The work done by a force on a displacement is given by the dot product:

Work=Fd.\text{Work} = \overrightarrow{F} \cdot \overrightarrow{d}.

Given the force

F=2i^+bj^+k^,\overrightarrow{F} = 2\hat{i} + b\hat{j} + \hat{k},

and the displacement

d=i^2j^k^,\overrightarrow{d} = \hat{i} - 2\hat{j} - \hat{k},

compute the dot product:

Fd=(2)(1)+(b)(2)+(1)(1).\overrightarrow{F} \cdot \overrightarrow{d} = (2)(1) + (b)(-2) + (1)(-1).

Simplify the expression:

Fd=22b1=12b.\overrightarrow{F} \cdot \overrightarrow{d} = 2 - 2b - 1 = 1 - 2b.

Since the work done is zero:

12b=0.1 - 2b = 0.

Solve for

bb

:

2b=1,2b = 1,
b=12.b = \frac{1}{2}.

Thus, the value of

bb

is

12\frac{1}{2}

, which corresponds to Option B.

Q93
A sand dropper drops sand of mass m(t) on a conveyer belt at a rate proportional to the square root of speed (v) of the belt, i.e., dmdtv\dfrac{dm}{dt} \propto \sqrt{v}. If P is the power delivered to run the belt at constant speed then which of the following relationship is true?
A P v\propto \sqrt{v}
B P v\propto v
C P2v3P^2 \propto v^3
D P2v5P^2 \propto v^5
Correct Answer
Option D
Solution

Given,

dmdtv{{dm} \over {dt}} \propto \sqrt v

So,

dmdt=kv{{dm} \over {dt}} = k\sqrt v

.... (i) where, k = constant We know, Power =

P=FVP = FV
P=dpdtv\Rightarrow P = {{dp} \over {dt}}v

(As

F=dpdtF = {{dp} \over {dt}}

where, p = linear momentum)

P=ddt(mv)v\Rightarrow P = {d \over {dt}}(mv)v
P=vdmdt.v\Rightarrow P = v{{dm} \over {dt}}\,.\,v

(As speed is constant i.e. v = constant)

P=v2(kv)\Rightarrow P = {v^2}(k\sqrt v )

[From (i)]

P=kv5/2\Rightarrow P = k{v^{5/2}}

by squaring both sides,

P2=k2v5\Rightarrow {P^2} = {k^2}{v^5}
P2v5\Rightarrow {P^2} \propto {v^5}

(As k2\mathrm{k^2} = constant) Hence, option 4 is correct.

Q94
A force F=α+βx2\mathrm{F}=\alpha+\beta \mathrm{x}^2 acts on an object in the x -direction. The work done by the force is 5 J when the object is displaced by 1 m . If the constant α=1 N\alpha=1 \mathrm{~N} then β\beta will be
A 15 N/m215 \mathrm{~N} / \mathrm{m}^2
B 10 N/m210 \mathrm{~N} / \mathrm{m}^2
C 12 N/m212 \mathrm{~N} / \mathrm{m}^2
D 8 N/m28 \mathrm{~N} / \mathrm{m}^2
Correct Answer
Option C
Solution

The work done by a force is given by the integral of the force over the displacement. The force is given by:

F(x)=α+βx2F(x) = \alpha + \beta x^2

To find the work done when the object is displaced from x=0x = 0 to x=1x = 1, we compute:

W=01(α+βx2)dxW = \int_{0}^{1} (\alpha + \beta x^2) \, dx

Substituting α=1N\alpha = 1 \, \text{N}:

W=01(1+βx2)dx=011dx+01βx2dxW = \int_{0}^{1} (1 + \beta x^2) \, dx = \int_{0}^{1} 1 \, dx + \int_{0}^{1} \beta x^2 \, dx

Calculating each integral separately: 011dx=[x]01=1 \int_{0}^{1} 1 \, dx = [x]_{0}^{1} = 1 01βx2dx=β[x33]01=β[133033]=β3 \int_{0}^{1} \beta x^2 \, dx = \beta \left[ \dfrac{x^3}{3} \right]_{0}^{1} = \beta \left[\dfrac{1^3}{3} - \dfrac{0^3}{3}\right] = \dfrac{\beta}{3} Thus, the total work done is:

W=1+β3W = 1 + \frac{\beta}{3}

We are given that the work done is 5 J, so:

1+β3=51 + \frac{\beta}{3} = 5

Subtract 1 from both sides:

β3=4\frac{\beta}{3} = 4

Multiply both sides by 3 to solve for β\beta:

β=12N/m2\beta = 12 \, \text{N/m}^2

Therefore, the value of β\beta is 12N/m2\boxed{12 \, \text{N/m}^2}.

Thus, Option C 12N/m212 \, \text{N/m}^2 is the correct answer.

Q95
Two bodies are having kinetic energies in the ratio 16 : 9. If they have same linear momentum, the ratio of their masses respectively is :
A 3:43: 4
B 4:34: 3
C 9:169: 16
D 16:916: 9
Correct Answer
Option C
Solution

The kinetic energy of a body of mass mm and velocity vv is given by K=12mv2K=\dfrac{1}{2}mv^2.

Since the bodies have the same linear momentum, we can write:

p=mvp=mv

where pp is the linear momentum of the bodies.

Let the masses of the two bodies be m1m_1 and m2m_2 and their kinetic energies be K1K_1 and K2K_2, respectively.

Then, we have:

K1K2=169\frac{K_1}{K_2}=\frac{16}{9}
12m1v12÷12m2v22=169\frac{1}{2}m_1v_1^2\div\frac{1}{2}m_2v_2^2=\frac{16}{9}

Since p=mvp=mv, we have v1=pm1v_1=\dfrac{p}{m_1} and v2=pm2v_2=\dfrac{p}{m_2}. Substituting these in the above equation, we get:

m2m1=916\frac{m_2}{m_1}=\frac{9}{16}

Therefore, the ratio of the masses of the two bodies is 9:16\boxed{9:16}.

Q96
A particle of mass M is moving in a circle of fixed radius R in such a way that its centripetal acceleration at time t is given by n2 R t2 where n is a constant. The power delivered to the particle by the force acting on it, is :
A M n2 R2 t
B M n R2 t
C M n R2 t2
D 12{1 \over 2} M n2 R2 t2
Correct Answer
Option A
Solution

We know, centripetal acceleration =

V2R{{{V^2}} \over R}

\therefore According to question,

V2R{{{V^2}} \over R}

=

n2Rt2{n^2}R{t^2}

\Rightarrow V2 = n2 R2 t2 \Rightarrow V = nRt \Rightarrow

dVdt{{dV} \over {dt}}

= nR Power (P) = Force (F) ×\times Velocity (V) = M

dVdt{{dV} \over {dt}}

(V) = M (nR) (nRt) = Mn2R2t

Q97
A wire suspended vertically from one of its ends is stretched by attaching a weight of 200N200N to the lower end. The weight stretches the wire by 11 mm.mm. Then the elastic energy stored in the wire is
A 0.20.2 JJ
B 1010 JJ
C 2020 JJ
D 0.10.1 JJ
Correct Answer
Option D
Solution

The elastic potential energy

=12×= {1 \over 2} \times

Force ×\times extension

=12×200×0.001=0.1J= {1 \over 2} \times 200 \times 0.001 = 0.1\,J
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