Work Power & Energy

JEE Physics · 82 questions · Page 8 of 9 · Click an option or "Show Solution" to reveal answer

Q71
The potential energy function (in JJ ) of a particle in a region of space is given as U=(2x2+3y3+2z)U=\left(2 x^2+3 y^3+2 z\right). Here x,yx, y and zz are in meter. The magnitude of xx-component of force (in NN ) acting on the particle at point P(1,2,3)mP(1,2,3) \mathrm{m} is :
A 4
B 2
C 8
D 6
Correct Answer
Option A
Solution

The force acting on a particle can be determined from the potential energy function by using the negative gradient.

In three-dimensional space, the force vector F is related to the potential energy function U U by:

F=U\mathbf{F} = -\nabla U

where U \nabla U (the gradient of U U ) is a vector with components given by the partial derivatives of U U with respect to x x , y y , and z z :

U=(Ux,Uy,Uz)\nabla U = \left( \frac{\partial U}{\partial x}, \frac{\partial U}{\partial y}, \frac{\partial U}{\partial z} \right)

Given the potential energy function:

U=2x2+3y3+2zU = 2x^2 + 3y^3 + 2z

Calculate the partial derivative of U U with respect to x x to find the x x -component of the force: Partial Derivative with respect to x x :

Ux=x(2x2+3y3+2z)=4x\frac{\partial U}{\partial x} = \frac{\partial}{\partial x}(2x^2 + 3y^3 + 2z) = 4x

Calculate the x x -component of the force: Since Fx=Ux F_x = -\dfrac{\partial U}{\partial x} , the x x -component of the force is:

Fx=4xF_x = -4x

Evaluate at point P(1,2,3) P(1,2,3) : Substitute x=1 x = 1 into the expression for Fx F_x :

Fx=4(1)=4F_x = -4(1) = -4

The magnitude of the x x -component of the force is:

Fx=4N|F_x| = 4 \, \text{N}

Thus, the correct answer is Option A: 4.

Q72
The potential energy of a 11 kgkg particle free to move along the xx-axis is given by V(x)=(x44x22)JV\left( x \right) = \left( {{{{x^4}} \over 4} - {{{x^2}} \over 2}} \right)J. The total mechanical energy of the particle is 2J.2J. Then, the maximum speed (in m/sm/s) is
A 32{3 \over {\sqrt 2 }}
B 2{\sqrt 2 }
C 12{1 \over {\sqrt 2 }}
D 22
Correct Answer
Option A
Solution

Velocity is maximum when kinetic energy is maximum and when kinetic energy is maximum then potential energy should be minimum For minimum potential energy,

dVdx=0{{dV} \over {dx}} = 0
x3x=0\Rightarrow {x^3} - x = 0
x=±1\Rightarrow x = \pm 1

\Rightarrow Min. Potential energy (P.E.) =

1412=14J{1 \over 4} - {1 \over 2} = - {1 \over 4}J
K.E.(max.)+P.E.(min.)=2K.E{._{\left( {\max .} \right)}} + P.E{._{\left( {\min .} \right)}} = 2\,

(Given) \therefore

K.E.(max.)=2+14=94K.E{._{\left( {\max .} \right)}} = 2 + {1 \over 4} = {9 \over 4}

\therefore

12mvmax2{1 \over 2}mv_{\max }^2

=

94{9 \over 4}
12×1×v2max.=94\Rightarrow {1 \over 2} \times 1 \times {v^2}_{\max .} = {9 \over 4}
vmax=32\Rightarrow {v_{\max }} = {3 \over {\sqrt 2 }}

m/s

Q73
A mass of MM kgkg is suspended by a weightless string. The horizontal force that is required to displace it until the string makes an angle of 45{45^ \circ } with the initial vertical direction is
A Mg(2+1)Mg\left( {\sqrt 2 + 1} \right)
B Mg2Mg\sqrt 2
C Mg2{{Mg} \over {\sqrt 2 }}
D Mg(21)Mg\left( {\sqrt 2 - 1} \right)
Correct Answer
Option D
Solution

From work energy theorem we can say, Work done by tension ++ work done by force (applied) ++ Work done by gravitational force == change in kinetic energy Here Work done by tension is zero

0+F×ABMg×AC=0\Rightarrow 0 + F \times AB - Mg \times AC = 0
F=Mg(ACAB)=Mg[11212]\Rightarrow F = Mg\left( {{{AC} \over {AB}}} \right) = Mg\left[ {{{1 - {1 \over {\sqrt 2 }}} \over {{1 \over 2}}}} \right]

[ as

AB=sin45=2AB = \ell \sin {45^ \circ } = {\ell \over {\sqrt 2 }}

and

AC=OCOA=cos45=(112)AC = OC - OA = \ell - \ell \,\cos \,{45^ \circ } = \ell \left( {1 - {1 \over {\sqrt 2 }}} \right)

where

=\ell =

length of the string. ]

F=Mg(21)\Rightarrow F = Mg\left( {\sqrt 2 - 1} \right)
Q74
Three bodies A, B and C have equal kinetic energies and their masses are 400 g,1.2 kg400 \mathrm{~g}, 1.2 \mathrm{~kg} and 1.6 kg1.6 \mathrm{~kg} respectively. The ratio of their linear momenta is :
A 1:3:21: \sqrt{3}: 2
B 3:2:1\sqrt{3}: \sqrt{2}: 1
C 1:3:21: \sqrt{3}: \sqrt{2}
D 2:3:1\sqrt{2} : \sqrt{3}: 1
Correct Answer
Option A
Solution

Given that the bodies A, B, and C have equal kinetic energies, we can use the relationship between kinetic energy (

K.E.K.E.

) and linear momentum (

pp

) to find the ratio of their momenta. Recall the formula for kinetic energy is

K.E.=12mv2K.E. = \frac{1}{2}mv^2

and the formula for momentum is

p=mvp = mv

, where

mm

is the mass and

vv

is the velocity of the object.

First, from the kinetic energy formula, we can express the velocity in terms of kinetic energy and mass:

v=2K.E.m.v = \sqrt{\frac{2 \cdot K.E.}{m}}.

The momentum can then be rewritten using the velocity expression obtained from the kinetic energy equation:

p=m2K.E.m=2mK.E..p = m\sqrt{\frac{2 \cdot K.E.}{m}} = \sqrt{2m \cdot K.E.}.

Given that the kinetic energies are the same for all three bodies, we can ignore the kinetic energy term when comparing the ratios, simplifying our comparison to the square root of their masses:

pm.p \propto \sqrt{m}.

Now, we calculate the ratio of their linear momenta using their masses.

Note that the masses should be in consistent units for a valid comparison, so we'll use kilograms for all: Mass of A =

400 g=0.4 kg400 \mathrm{~g} = 0.4 \mathrm{~kg}

Mass of B =

1.2 kg1.2 \mathrm{~kg}

Mass of C =

1.6 kg1.6 \mathrm{~kg}

Thus, the ratio of their momenta will be proportional to the square root of their masses:

Ratio of momenta=0.4:1.2:1.6=410:1210:1610=25:65:85.\text{Ratio of momenta} = \sqrt{0.4} : \sqrt{1.2} : \sqrt{1.6} = \sqrt{\frac{4}{10}} : \sqrt{\frac{12}{10}} : \sqrt{\frac{16}{10}} = \sqrt{\frac{2}{5}} : \sqrt{\frac{6}{5}} : \sqrt{\frac{8}{5}}.

Simplifying these we get:

Ratio of momenta=25:65:85=2:6:8.\text{Ratio of momenta} = \frac{\sqrt{2}}{\sqrt{5}} : \frac{\sqrt{6}}{\sqrt{5}} : \frac{\sqrt{8}}{\sqrt{5}} = \sqrt{2} : \sqrt{6} : \sqrt{8}.

Recognizing that

6\sqrt{6}

is equivalent to

23\sqrt{2} \cdot \sqrt{3}

and that

8\sqrt{8}

is equivalent to

222=22\sqrt{2} \cdot \sqrt{2} \cdot \sqrt{2} = 2\sqrt{2}

, we see this can also be expressed as:

2:23:22.\sqrt{2} : \sqrt{2} \cdot \sqrt{3} : 2\sqrt{2}.

Dividing through by

2\sqrt{2}

to simplify the ratio, the final ratio of their linear momenta is:

1:3:2,1 : \sqrt{3} : 2,

which matches Option A

1:3:2.1: \sqrt{3}: 2.
Q75
Identify the correct statements from the following : A. Work done by a man in lifting a bucket out of a well by means of a rope tied to the bucket is negative. B. Work done by gravitational force in lifting a bucket out of a well by a rope tied to the bucket is negative. C. Work done by friction on a body sliding down an inclined plane is positive. D. Work done by an applied force on a body moving on a rough horizontal plane with uniform velocity is zero. E. Work done by the air resistance on an oscillating pendulum is negative. Choose the correct answer from the options given below :
A A and C only
B B and D only
C B, D and E only
D B and E only
Correct Answer
Option D
Solution

When a man lifts a bucket out of a well using a rope, work is done by the man and the gravitational force.

The work done by the man is positive as he has to exert an upward force to lift the bucket.

The work done by the gravitational force is negative because the direction of the force is opposite to the direction of displacement.

Therefore, the statement (A) "Work done by a man in lifting a bucket out of a well by means of rope tied to the bucket is negative." is incorrect.

Therefore, the statement (B) "Work done by gravitational force in lifting a bucket out of a well by a rope tied to the bucket is negative." is correct.

Work is defined as the product of force and displacement in the direction of the force.

When a body slides down an inclined plane, the force of friction acts against the motion of the body, opposing its descent.

The direction of the force of friction is opposite to the direction of the displacement of the body, which is downwards.

Hence, the work done by the force of friction is negative.

Therefore, the statement (C) "Work done by friction on a body sliding down an inclined plane is positive" is incorrect.

If the body is moving on a rough horizontal plane, there will be friction present, which will act in the opposite direction to the applied force.

The force of friction will oppose the motion of the body, reducing its velocity.

As a result, the net work done on the body will not be zero, as the force of friction and the applied force will not cancel each other out completely.

Therefore, the statement (D) "Work done by an applied force on a body moving on a rough horizontal plane with uniform velocity is zero." is incorrect.

Statement E: "Work done by the air resistance on an oscillating pendulum is negative."

This statement refers to the work done by the air resistance on an oscillating pendulum, which is a physical system that swings back and forth under the influence of gravity.

As the pendulum oscillates, it experiences air resistance, which opposes its motion and slows it down.

The direction of the air resistance force is opposite to the direction of the displacement of the pendulum, which is back and forth.

Hence, the work done by the air resistance force is negative, as the direction of the force and the displacement are opposite.

Therefore, the statement (E) "Work done by the air resistance on an oscillating pendulum is negative" is correct.

Q76
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.

Q77
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.

Q78
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.

Q79
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.

Q80
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}.

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