Work Power & Energy

JEE Physics · 82 questions · Page 2 of 9 · Click an option or "Show Solution" to reveal answer

Q11
A body of mass mm is accelerated uniformly from rest to a speed vv in a time T.T. The instantaneous power delivered to the body as a function of time is given by
A mv2T2.t2{{m{v^2}} \over {{T^2}}}.{t^2}
B mv2T2.t{{m{v^2}} \over {{T^2}}}.t
C 12mv2T2.t2{1 \over 2}{{m{v^2}} \over {{T^2}}}.{t^2}
D 12mv2T2.t{1 \over 2}{{m{v^2}} \over {{T^2}}}.t
Correct Answer
Option B
Solution
u=0;v=u+aT;v=aTu = 0;v = u + aT;v = aT

Instantaneous power

=F×v=m.a.at=m.a2.t= F \times v = m.\,a.\,at = m.{a^2}.t

\therefore Instantaneous power

=mv2tT2= {{m{v^2}t} \over {{T^2}}}
Q12
The upper half of an inclined plane with inclination ϕ\phi is perfectly smooth while the lower half is rough. A body starting from rest at the top will again come to rest at the bottom if the coefficient of friction for the lower half is given by
A 2cosϕ2\,\cos \,\,\phi
B 2sinϕ2\,sin\,\,\phi
C tanϕ\,\tan \,\,\phi
D 2tanϕ2\,\tan \,\,\phi
Correct Answer
Option D
Solution

Let the length of the inclined plane is =

ll

. So only

l2{l \over 2}

part will have friction. According to work-energy theorem,

W=Δk=0W = \Delta k = 0

(Since initial and final speeds are zero) \therefore Work done by friction + Work done by gravity

=0=0

i.e.,

(μmgcosϕ)2+mgsinϕ=0- \left( {\mu \,mg\,\cos \,\phi } \right){\ell \over 2} + mg\ell \,\sin \,\phi = 0

or

μ2cosϕ=sinϕ{\mu \over 2}\cos \,\phi = \sin \phi

or

μ=2tanϕ\mu = 2\,\tan \,\phi
Q13
A 22 kgkg block slides on a horizontal floor with a speed of 4m/s.4m/s. It strikes a uncompressed spring, and compress it till the block is motionless. The kinetic friction force is 15N15N and spring constant is 10,00010, 000 N/m.N/m. The spring compresses by
A 8.5cm8.5cm
B 5.5cm5.5cm
C 2.5cm2.5cm
D 11.0cm11.0cm
Correct Answer
Option B
Solution

Let the block compress the spring by

xx

before coming to rest.

Initial kinetic energy of the block == (potential energy of compressed spring) ++ work done due to friction.

12×2×(4)2=12×10000×x2+15×x{1 \over 2} \times 2 \times {\left( 4 \right)^2} = {1 \over 2} \times 10000 \times {x^2} + 15 \times x
10,000x2+30x32=010,000{x^2} + 30x - 32 = 0
5000x2+15x16=0\Rightarrow 5000{x^2} + 15x - 16 = 0

\therefore

x=15±(15)24×(5000)(16)2×5000x = {{ - 15 \pm \sqrt {{{\left( {15} \right)}^2} - 4 \times \left( {5000} \right)\left( { - 16} \right)} } \over {2 \times 5000}}
=0.055m=5.5cm.\,\,\,\,\, = 0.055m = 5.5cm.
Q14
An athlete in the olympic games covers a distance of 100100 mm in 1010 s.s. His kinetic energy can be estimated to be in the range
A 200J500J200J-500J
B 2×105J3×105J2 \times {10^5}J - 3 \times {10^5}J
C 20,000J50,000J20,000J - 50,000J
D 2,000J5,000J2,000J - 5,000J
Correct Answer
Option D
Solution

The average speed of the athelete

v=10010=10m/sv = {{100} \over {10}} = 10m/s\,\,\,\,

\therefore

K.E.=12mv2K.E. = {1 \over 2}m{v^2}

If mass of athlete is

4040
kgkg

then,

K.E.K.E.
=12×40×(10)2=2000J= {1 \over 2} \times 40 \times {\left( {10} \right)^2} = 2000J

If mass of athlete is

100100
kgkg

then,

K.E.K.E.
=12×100×(10)2=5000J= {1 \over 2} \times 100 \times {\left( {10} \right)^2} = 5000J

His kinetic energy can be in the range = 2000 J to 5000 J.

Q15
A porter lifts a heavy suitcase of mass 80 kg and at the destination lowers it down by a distance of 80 cm with a constant velocity. Calculate the work done by the porter in lowering the suitcase. (take g = 9.8 ms-2)
A +627.2 J
B -62720.0 J
C -627.2 J
D 784.0 J
Correct Answer
Option C
Solution
W=N×ΔxW = - N \times \Delta x
=80×9.8×80100= - 80 \times 9.8 \times {{80} \over {100}}
=627.2= - 627.2

J

Q16
A time dependent force F = 6t acts on a particle of mass 1 kg. If the particle starts from rest, the work done by the force during the first 1 sec. will be:
A 18 J
B 4.5 J
C 22 J
D 9 J
Correct Answer
Option B
Solution

Given that, F = 6t We know, F = ma =

mdvdtm{{dv} \over {dt}}

\therefore

mdvdt=6tm{{dv} \over {dt}} = 6t

\Rightarrow

1.dvdt=6t1.{{dv} \over {dt}} = 6t

[as m = 1] \Rightarrow

0vdv=6tdt\int\limits_0^v {dv} = \int {6t} dt

\Rightarrow

v=6[t22]01v = 6\left[ {{{{t^2}} \over 2}} \right]_0^1

\Rightarrow

v=62=3v = {6 \over 2} = 3

m/s [ as given t = 1 sec ] Work done by the body during the first 1 form work-energy theorem, W =

Δ\Delta

K.E =

12m(V2v2){1 \over 2}m\left( {{V^2} - {v^2}} \right)

=

12.1.(3202){1 \over 2}.1.\left( {{3^2} - {0^2}} \right)

= 4.5 J

Q17
A uniform cable of mass 'M' and length 'L' is placed on a horizontal surface such that its (1/n)th part is hanging below the edge of the surface. To lift the hanging part of the cable upto the surface, the work done should be :
A 2MgLn2{{2MgL} \over {{n^2}}}
B nMgL
C MgL2n2{{MgL} \over {2{n^2}}}
D MgLn2{{MgL} \over {{n^2}}}
Correct Answer
Option C
Solution

To solve this problem, we need to determine the work done to lift the hanging part of the cable up to the surface.

The work done lifting a small element of the cable will be the weight of the element times the distance it has to be lifted.

Let's take a small section of the cable at a depth xx below the surface.

This section has a length of dxdx, so its mass is (M/L)dx(M/L)dx where (M/L)(M/L) is the linear mass density of the cable.

The work dWdW done to lift this small section up to the surface is the weight of the section times the distance it has to be lifted : dW=(M/L)gdx×xdW = (M/L)gdx \times x.

Integrating this expression from 0 to L/n (the length of the hanging part of the cable) gives the total work done :

W=0L/n(M/L)gxdxW = \int\limits_{0}^{L/n} (M/L)gxdx
=(Mg/L)0L/nxdx= (Mg/L) \int\limits_{0}^{L/n} xdx
=(Mg/L)×[x2/2]0L/n= (Mg/L) \times [x^2/2]_{0}^{L/n}
=(Mg/L)×[L2/(2n2)]= (Mg/L) \times [L^2/(2n^2)]
=MgL/(2n2)= MgL/(2n^2)

So the work done to lift the hanging part of the cable up to the surface is MgL/(2n2)MgL/(2n^2).

Therefore, the correct answer is Option C :

MgL2n2\frac{MgL}{2n^2}
Q18
If the potential energy between two molecules is given by U = Ar6+Br12 - {A \over {{r^6}}} + {B \over {{r^{12}}}}, then at equilibrium, separation between molecules, and the potential energy are :
A (2BA)1/6{\left( {{{2B} \over A}} \right)^{1/6}}, A24B - {{{A^2}} \over {4B}}
B (2BA)1/6,A22B{\left( {{{2B} \over A}} \right)^{1/6}}, - {{{A^2}} \over {2B}}
C (BA)1/6,0{\left( {{B \over A}} \right)^{1/6}},0
D (B2A)1/6,A22B{\left( {{B \over {2A}}} \right)^{1/6}}, - {{{A^2}} \over {2B}}
Correct Answer
Option A
Solution

U =

Ar6+Br12- {A \over {{r^6}}} + {B \over {{r^{12}}}}

F = -

dUdr{{dU} \over {dr}}

= – (A(–6r–7 )) + B(–12r–13) for equilibrium, F = 0 \therefore 0 =

6Ar712Br13{{6A} \over {{r^7}}} - {{12B} \over {{r^{13}}}}

\Rightarrow

6A12B=1r6{{6A} \over {12B}} = {1 \over {{r^6}}}

\Rightarrow r =

(2BA)16{\left( {{{2B} \over A}} \right)^{{1 \over 6}}}

\therefore U =

A2BA+B(2BA)2- {A \over {{{2B} \over A}}} + {B \over {{{\left( {{{2B} \over A}} \right)}^2}}}

=

A22B+A24B- {{{A^2}} \over {2B}} + {{{A^2}} \over {4B}}

=

A24B- {{{A^2}} \over {4B}}
Q19
A person pushes a box on a rough horizontal plateform surface. He applies a force of 200 N over a distance of 15 m. Thereafter, he gets progressively tired and his applied force reduces linearly with distance to 100 N. The total distance through which the box has been moved is 30 m. What is the work done by the person during the total movement of the box?
A 5690 J
B 5250 J
C 2780 J
D 3280 J
Correct Answer
Option B
Solution

Work done = area of ABCEO = area of trapezium ABCD + area of rectangle ODCE =

12{1 \over 2}

×\times 45 ×\times 30 + 100 ×\times 30 = 5250J

Q20
A 60 HP electric motor lifts an elevator having a maximum total load capacity of 2000 kg. If the frictional force on the elevator is 4000 N, the speed of the elevator at full load is close to : (1 HP = 746 W, g = 10 ms-2)
A 1.5 ms-1
B 1.7 ms-1
C 2.0 ms-1
D 1.9 ms-1
Correct Answer
Option D
Solution

F = mg + f F = 20000 + 4000 = 24000 N We know, Power(P) = Fv \Rightarrow v =

PF{P \over F}

=

60×74624000{{60 \times 746} \over {24000}}

\Rightarrow v \approx 1.9 m/s

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