1) A gravity-free hall contains a tray of mass M carrying a cubical block of ice of mass m and edge L at rest in the middle. If the ice melts, the centre of mass of the tray plus ice system will descend by a distance that can be calculated.
2) Two people of masses 50 kg and 60 kg sitting at opposite ends of a 4 m long, 40 kg boat discuss a mechanics problem and move to the middle. Neglecting friction, the displacement of the boat in the water can be calculated.
3) A cart of mass M recoils with speed v backward on frictionless rails when a man of mass m starts moving towards the engine on the cart. The
Real Time Code Generation for Nonlinear Model Predictive ControlBehzad Samadi
This is a quick introduction to optimal control and nonlinear model predictive control. It also includes code generation for a NMPC controller. For a recorded webinar, follow this link: http://goo.gl/c5zFgN
Response of dynamic systems to harmonic excitation is discussed. Single degree of freedom systems are considered. For general damped multi degree of freedom systems, see my book Structural Dynamic Analysis with Generalized Damping Models: Analysis (e.g., in Amazon http://buff.ly/NqwHEE)
Super-twisting sliding mode based nonlinear control for planar dual arm robotsjournalBEEI
In this paper, a super-twisting algorithm sliding mode controller is proposed for a planar dual arm robot. The control strategy for the manipulator system can effectively counteract chattering phenomenon happened with conventional sliding mode approach. The modeling is implemented in order to provide the capability of maneuvering object in translational and rotational motions. The control is developed for a 2n-link robot and subsequently simulations is carried out for a 4-link system. Comparative numerical study shows that the designed controller performance with good tracking ability and smaller chattering compared with basic sliding mode controller.
Robust model predictive control for discrete-time fractional-order systemsPantelis Sopasakis
In this paper we propose a tube-based robust model predictive control scheme for fractional-order discrete-
time systems of the Grunwald-Letnikov type with state and input constraints. We first approximate the infinite-dimensional fractional-order system by a finite-dimensional linear system and we show that the actual dynamics can be approximated arbitrarily tight. We use the approximate dynamics to design a tube-based model predictive controller which endows to the controlled closed-loop system robust stability properties
This paper is my work on Einstein's Relativity theory for speed greater than light.The paper mainly focus on to generalize the Lorentz factor , equation of negative energy and negative mass thus proving the existence of wormholes and the derivation of new space metric.
STRESS ANALYSIS OF TRACTOR’S FRONT-END BUCKET USING MOHR'S CIRCLEWahid Dino Samo
To better understand the stress state for a new tractor, a structural analysis computer program was used to determine stresses in the tractor's front-end bucket. For the location shown, it was determined that the stresses are σx = 30 psi, σy = 10 psi, and τxy = 20 psi
Using Mohr's circle, what is
1) the principal direction and principal normal stresses
2) maximum shear direction and the maximum shearing stress.
APPROACH:
Construct the basic Mohr's circle for the given stress state.
Determine the principal direction from the Mohr's circle diagram, and then the principal stresses.
Find the maximum shear stress direction from the Mohr's circle diagram.
Discusses projectile motion as two dimensional motion.
**More good stuff available at:
www.wsautter.com
and
http://www.youtube.com/results?search_query=wnsautter&aq=f
Real Time Code Generation for Nonlinear Model Predictive ControlBehzad Samadi
This is a quick introduction to optimal control and nonlinear model predictive control. It also includes code generation for a NMPC controller. For a recorded webinar, follow this link: http://goo.gl/c5zFgN
Response of dynamic systems to harmonic excitation is discussed. Single degree of freedom systems are considered. For general damped multi degree of freedom systems, see my book Structural Dynamic Analysis with Generalized Damping Models: Analysis (e.g., in Amazon http://buff.ly/NqwHEE)
Super-twisting sliding mode based nonlinear control for planar dual arm robotsjournalBEEI
In this paper, a super-twisting algorithm sliding mode controller is proposed for a planar dual arm robot. The control strategy for the manipulator system can effectively counteract chattering phenomenon happened with conventional sliding mode approach. The modeling is implemented in order to provide the capability of maneuvering object in translational and rotational motions. The control is developed for a 2n-link robot and subsequently simulations is carried out for a 4-link system. Comparative numerical study shows that the designed controller performance with good tracking ability and smaller chattering compared with basic sliding mode controller.
Robust model predictive control for discrete-time fractional-order systemsPantelis Sopasakis
In this paper we propose a tube-based robust model predictive control scheme for fractional-order discrete-
time systems of the Grunwald-Letnikov type with state and input constraints. We first approximate the infinite-dimensional fractional-order system by a finite-dimensional linear system and we show that the actual dynamics can be approximated arbitrarily tight. We use the approximate dynamics to design a tube-based model predictive controller which endows to the controlled closed-loop system robust stability properties
This paper is my work on Einstein's Relativity theory for speed greater than light.The paper mainly focus on to generalize the Lorentz factor , equation of negative energy and negative mass thus proving the existence of wormholes and the derivation of new space metric.
STRESS ANALYSIS OF TRACTOR’S FRONT-END BUCKET USING MOHR'S CIRCLEWahid Dino Samo
To better understand the stress state for a new tractor, a structural analysis computer program was used to determine stresses in the tractor's front-end bucket. For the location shown, it was determined that the stresses are σx = 30 psi, σy = 10 psi, and τxy = 20 psi
Using Mohr's circle, what is
1) the principal direction and principal normal stresses
2) maximum shear direction and the maximum shearing stress.
APPROACH:
Construct the basic Mohr's circle for the given stress state.
Determine the principal direction from the Mohr's circle diagram, and then the principal stresses.
Find the maximum shear stress direction from the Mohr's circle diagram.
Discusses projectile motion as two dimensional motion.
**More good stuff available at:
www.wsautter.com
and
http://www.youtube.com/results?search_query=wnsautter&aq=f
Breb recruitment (Mechanical) question and solutions(8th june 2018)Alamin Md
Bangladesh Rural Electrification Board's recruitment exam was held on 8th June 2018. Here is the solution of mechanical engineering question. Exam was held in MIST.
Hope this will be a great help to those who wants to do better in engineering job field of Bangladesh.
Model Attribute Check Company Auto PropertyCeline George
In Odoo, the multi-company feature allows you to manage multiple companies within a single Odoo database instance. Each company can have its own configurations while still sharing common resources such as products, customers, and suppliers.
Acetabularia Information For Class 9 .docxvaibhavrinwa19
Acetabularia acetabulum is a single-celled green alga that in its vegetative state is morphologically differentiated into a basal rhizoid and an axially elongated stalk, which bears whorls of branching hairs. The single diploid nucleus resides in the rhizoid.
Instructions for Submissions thorugh G- Classroom.pptxJheel Barad
This presentation provides a briefing on how to upload submissions and documents in Google Classroom. It was prepared as part of an orientation for new Sainik School in-service teacher trainees. As a training officer, my goal is to ensure that you are comfortable and proficient with this essential tool for managing assignments and fostering student engagement.
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
Embracing GenAI - A Strategic ImperativePeter Windle
Artificial Intelligence (AI) technologies such as Generative AI, Image Generators and Large Language Models have had a dramatic impact on teaching, learning and assessment over the past 18 months. The most immediate threat AI posed was to Academic Integrity with Higher Education Institutes (HEIs) focusing their efforts on combating the use of GenAI in assessment. Guidelines were developed for staff and students, policies put in place too. Innovative educators have forged paths in the use of Generative AI for teaching, learning and assessments leading to pockets of transformation springing up across HEIs, often with little or no top-down guidance, support or direction.
This Gasta posits a strategic approach to integrating AI into HEIs to prepare staff, students and the curriculum for an evolving world and workplace. We will highlight the advantages of working with these technologies beyond the realm of teaching, learning and assessment by considering prompt engineering skills, industry impact, curriculum changes, and the need for staff upskilling. In contrast, not engaging strategically with Generative AI poses risks, including falling behind peers, missed opportunities and failing to ensure our graduates remain employable. The rapid evolution of AI technologies necessitates a proactive and strategic approach if we are to remain relevant.
Welcome to TechSoup New Member Orientation and Q&A (May 2024).pdfTechSoup
In this webinar you will learn how your organization can access TechSoup's wide variety of product discount and donation programs. From hardware to software, we'll give you a tour of the tools available to help your nonprofit with productivity, collaboration, financial management, donor tracking, security, and more.
Unit 8 - Information and Communication Technology (Paper I).pdfThiyagu K
This slides describes the basic concepts of ICT, basics of Email, Emerging Technology and Digital Initiatives in Education. This presentations aligns with the UGC Paper I syllabus.
The French Revolution, which began in 1789, was a period of radical social and political upheaval in France. It marked the decline of absolute monarchies, the rise of secular and democratic republics, and the eventual rise of Napoleon Bonaparte. This revolutionary period is crucial in understanding the transition from feudalism to modernity in Europe.
For more information, visit-www.vavaclasses.com
The French Revolution Class 9 Study Material pdf free download
Center of mass hcv
1. BMSAPB.M.SHARMA ACADEMY OF PHYSICS
1
A-PDFPPTTOPDFDEMO:Purchasefromwww.A-PDF.comtoremovethewatermark
1
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2. Consider a gravity- free hall in which a tray of mass M,
carrying a cubical block of ice of mass m and edge L, is
at rest in the middle . If the ice melts, by what distance
does the centre of mass of “ the tray plus the ice”
system descend ?
2
Problem 10.Problem 10.
M m
L
2
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3. Problem 12.Problem 12.
Mr. Verma (50 kg) and Mr. Mathur (60 kg) are sitting at
the two extremes of a 4 m long boat (40 kg) standing
still in water. To discuss a mechanics problem, they
come to the middle of the boat.
3
Neglecting friction with water, how far does the boat
move in the water during the process ?
Solution.Solution. Let displacement of the boat is xb = X
Mr Verma Mr Mathur
(40 kg)
(50 kg) (60 kg)
4m
3
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4. As no external forces are acting on the system the
displacement of centre of mass of the system should be
zero.
0 0
( )
+ ++ ++ ++ +
====
+ ++ ++ ++ +
V V M M
cm
b v m
M x M x M x
x
M M M
40 50( 2) 60( 2)
0
150
x x× + + + −× + + + −× + + + −× + + + −
⇒ =⇒ =⇒ =⇒ =
13x m⇒ =⇒ =⇒ =⇒ =
The displacement of Mr. Verma,Xv = (x + 2) m
The displacement of Mr. Mathur,Xm = (x - 2) m
4
4
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5. Problem 13.Problem 13.
A cart of mass M is at rest on a frictionless horizontal
surface and a pendulum bob of mass m hangs from the
roof of the cart . The string breaks, the bob falls on the
floor, makes several collisions on the floor and finally
lands up in a small slot made in the floor. The
horizontal distance between the string and the slot is L.
5
Find the displacement of the cart during this process.
5
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6. Solution.Solution.
Let displacement of cart
cx x= −= −= −= −
Displacement of bob
( )bx L X= −= −= −= −
( ) 0cm systemx ====
. 0cart cart bob bobM x M x+ =+ =+ =+ =
.( ) ( ) 0M x m L X− + − =− + − =− + − =− + − =
mL
x
m M
====
++++
m
M
L
m
M
L
(-x)
6
6
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7. Problem 19.Problem 19.
A man of mass M having a bag of mass m slips from the
roof of a tall building of height H and starts falling
vertically. When at a height h from the ground, he
notices that the ground below him is pretty hard, but
there is a pond at a horizontal distance x from the line
of fall.
7
In order to save himself he throws the bag horizontally
(with respect to himself) in the direction opposite to the
pond.
Calculate the minimum horizontal velocity imparted to
the bag so that the man lands in the water. If the man
just succeeds to avoid the hard ground, where will the
bag land ?
7
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9. To avoid the man falling
on hard floor the man
should be displaced by a
horizontal displacement x
during which he fall a
height h.
Solution.Solution.
Considering (man + bag) as a system; No external
forces in horizontal direction is acting on man.
H
h
pond
x
9
9
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10. . 0man bagman bagM V M V
→ →→ →→ →→ →
+ =+ =+ =+ =
0b
x
M mv
t
− =− =− =− =
The time taken by man to fall a height h
T = time to fall H – time to fall (H – h)
2 2( )H H h
t
g g
−−−−
= == == == =
Hence horizontal velocity of man required
man
x
V
t
====
As no external force in horizontal direction hence, the
linear momentum of ‘man + bag’ system should be
conserved (i.e. equal to zero).
10
…(i)
10
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11. .bag
M x
v
m t
====
[ 2 2( 2)]
bag
Mx g
v
m H H
⇒ =⇒ =⇒ =⇒ =
− −− −− −− −
The displacement of centre of mass of “bag + Man”
system should be zero.
0man bagmanM x m x
→→→→ →→→→
+ =+ =+ =+ =
0bagMx mx⇒ − =⇒ − =⇒ − =⇒ − =
bag
Mx
x
m
⇒ =⇒ =⇒ =⇒ =
11
11
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12. Problem 20.Problem 20.
A ball of a mass 50 g moving at a speed of 2.0 m/s
strikes a plane surface at an angle of incidence 450. The
ball is reflected by the plane at equal angle of reflection
with the same speed.
12
Calculate
(a) the magnitude of the change in momentum of the
ball
(b) the change in the magnitude of the momentum of
the ball.
Solution.Solution.
(a) The momentum of the
ball just before striking
v v
m
m
45
0
45
0
12
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13. Change in linear momentum, final initialp p p
→→→→→→→→ →→→→
∆ = −∆ = −∆ = −∆ = −
0 ˆ2 cos45p mv j∆ =∆ =∆ =∆ =
| | 2p mv⇒ ∆ =⇒ ∆ =⇒ ∆ =⇒ ∆ =
0.14 /p kg m s⇒ ∆ =⇒ ∆ =⇒ ∆ =⇒ ∆ =
| | | |initial finalp p
→→→→ →→→→
====(b) As,
Hence, no change in linear momentum of the ball.
0 0ˆ ˆsin45 cos45initialp mv i mv j
→→→→
= −= −= −= −
0 0ˆ ˆsin45 cos45finalp mv i mv j
→→→→
= += += += +
13
13
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14. Problem 21.Problem 21.
Light in certain cases may be considered as a stream of
particles called photons. Each photon has a linear
momentum h/λ where h is the Planck’s constant and λ is
the wavelength of the light. A beam of light of
wavelength λ is incident on the plane mirror at an angle
of incidence θ.
14
Calculate the change in the linear momentum of a
photon as the beam is reflected by the mirror.
Solution.Solution.
No change in linear
momentum parallel to
mirror but there will be
change in linear
momentum in the direction
normal to mirror.
p =
λ
h
p =
λ
h
θ θ
14
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16. Problem 24.Problem 24.
During a heavy rain, hailstones of average size 1.0 cm in
diameter fall with an average speed of 20 m/s. Suppose
2000 hailstones strike every square meter of a 10 m ×
10 m roof perpendicularly in one second and assume
that the hailstones do not rebound.
16
Calculate the average force exerted by the falling
hailstones on the roof. Density of the hailstones is 900
kg/m3.
Solution.Solution. Force applied by hail stone
| | t lmv mvp
F
t t
−−−−∆∆∆∆
= == == == =
∆ ∆∆ ∆∆ ∆∆ ∆
0
| | l lmv mv
F
t t
−−−−
= == == == =
∆ ∆∆ ∆∆ ∆∆ ∆
16
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18. Problem 25.Problem 25.
A ball of mass m is dropped onto a floor from a certain
height. The collision is perfectly elastic and the ball
rebounds to the same height and again falls.
18
Find the average force exerted by the ball on the floor
during a long time interval.
18
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19. Problem 26.Problem 26.
A railroad car of mass M is at rest on frictionless rails
when a man of mass m starts moving on the car towards
the engine. If the car recoils with a speed v backward on
the rails, with what velocity is the man approaching the
engine ?
19
Solution.Solution.
As linear momentum of car + man system in horizontal
direction will remain constant (i.e., will be zero)
vm,c
m
Engine
M
v
19
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20. ,( ) ( ) 0m cm v v M v− + − =− + − =− + − =− + − =
, ( )m cmv m M v⇒ = +⇒ = +⇒ = +⇒ = +
,
( )
m c
m M
v v
m
++++
⇒ =⇒ =⇒ =⇒ =
20
20
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21. Problem 27.Problem 27.
A gun is mounted on a railroad car. The mass of the car,
the gun, the shells and the operator is 50 m where m is
the mass of one shell. If the muzzle velocity of the
shells is 200 m/s, what is the recoil speed of the car
after the second shot ? Neglect friction.
21
Solution.Solution.
Taking Gun and car as a system no external force are
acting on the system in horizontal direction at any
time.
v1
gun vs,g
=200 m/s
21
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23. Problem 28.Problem 28.
Two persons each of mass m are standing at the two
extremes of a railroad car of mass M resting on a smooth
track. The person on left jumps to the left with a
horizontal speed u with respect to the state of the car
before the jump.
23
Thereafter, the other person jumps to the right, again
with the same horizontal speed u with respect to the
state of the car before his jump.
Find the velocity of the car after both the persons have
jumped off.
23
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24. Solution.Solution.
Considering both man and car as a system.
Initially the linear
momentum of the
system is zero.
1 10 ( ) ( )m v u M m v= − + += − + += − + += − + +
1
2
mu
v
M m
====
++++
Now, taking II man and car as a system
Initially linear momentum of the system is
…(i)
v1
24
24
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25. As, pinitial = pfinal
1( ) ( )
( 2 )initial
mu
p m M v m M
M m
= + = += + = += + = += + = +
++++
2 2( )finalp m u v Mv= + += + += + += + +
…(ii)
…(iii)
Now taking II man and car as a system
Initially linear momentum of the system is
v2
25
25
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26. 2 2( ) ( )
( 2 )
mu
m M m u v Mv
M m
+ = + ++ = + ++ = + ++ = + +
++++
2
2
( 2 )( )
m u
v
M m m M
⇒ = −⇒ = −⇒ = −⇒ = −
+ ++ ++ ++ +
Hence, the car will move with velocity
2
( 2 )( )
m u
M m m M+ ++ ++ ++ +
towards left.
26
26
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27. Problem 29.Problem 29.
Figure shows a small block of mass m which is started
with a speed v on the horizontal part of the bigger block
of mass M placed on a horizontal floor. The curved part
of the surface shown is semicircular. All the surfaces are
frictionless.
27
Find the speed of the bigger block when the smaller
block reaches the point A of the surface.
A
v
m
27
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28. Solution.Solution.
Considering bigger block
and smaller block as a
system.
The system has no force in
horizontal direction.
As surface of M is smooth
i.e. no friction between M &
m. Hence the bigger block
will start moving when m
reaches at the semicircular
track.
When “m” reaches at A, the ‘m’ block will move in
vertical direction and in horizontal direction both M and
m will move with same velocity (v).
A v
m
A
v’
v
28
28
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29. initialp mv====
( )finalp m M v= += += += +
initial finalp p⇒ =⇒ =⇒ =⇒ = mv
v
M m
⇒ =⇒ =⇒ =⇒ =
++++
Considering the linear momentum of the system in
horizontal direction.
29
29
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30. Problem 30.Problem 30.
In a typical Indian Bugghi (a luxury cart drawn by
horses), a wooden plate is fixed on the rear on which
one person can sit. A bugghi of mass 200 kg is moving
at a speed of 10 km/hr. As it overtakes a school boy
walking at a speed of 4 km/hr, the boy sits on the
wooden plate.
30
If the mass of the boy is 25 kg, what will be the new
velocity of the bugghi ?
Solution.Solution.
Considering the ‘Bugghi + School boy’ a system
200 10 25 4initialp = × + ×= × + ×= × + ×= × + ×
(200 25)finalp V= ×= ×= ×= ×
30
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32. Problem 33.Problem 33.
Consider a head- on collision between two particles of
masses m1 and m2. The initial speeds of the particles
are u1 and u2 in the same direction. The collision starts
at t = 0 and the particles interact for a time interval ∆t.
During the collision, the speed of the first particle varies
as
32
Find the speed of the second particle as a function of
time during the collision.
1 1 1
1
( ) ( )t u u
t
υ = + υ −υ = + υ −υ = + υ −υ = + υ −
∆∆∆∆
32
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33. Problem 34.Problem 34.
A bullet of mass m moving at a speed v hits a ball of
mass M kept at rest. A small part having mass ‘m’
breaks from the ball and sticks to the bullet. The
remaining ball is found to move at a speed v1 in the
direction of the bullet.
33
Find the velocity of the bullet after the collision.
33
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34. Problem 38.Problem 38.
Two friends A and B (each weighing 40 kg) are sitting
on a frictionless platform some distance d apart. A rolls
a ball of mass 4 kg on the platform towards B which B
catches. Then B rolls the ball toward A and A catches it.
The ball keeps on moving back and forth between A and
B. The ball has a fixed speed of 5 m/s on the platform.
34
(a) Find the speed of A after he rolls the ball for the first
time.
(b) Find the speed of A after he catches the ball for the
first time.
(c) Find the speed of A and B after the ball has made 5
round trips and is held by A.
(d) How many times can A roll the ball ?
(e) Where is the centre of mass of the system “ A + B +
ball” at the end of the nth trip ?
34
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35. 35
p = 20kg m/sA
20 kg m/s
A
20kg m/s
B
p =
40kg m/s
A,1
20kg m/s 40kg m/s
Solution.Solution.
After every throw ‘A’ or ‘B’ gain the momentum 20
kg/m/s in the direction opposite to the motion of ball.
Ist round
p = 20kg m/sA
m = p = 20 kg m/sball ballv ball
BA
35
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36. At the end of each round both the man receive a
momentum 40 kg m/s.
(a) pA = 20 = 40 vA
1
/
2Av m s====
p = 60kg m/sA
20 kg m/s
A
40kg m/s
B
20kg m/s
p =
80kg m/s
A,2
20kg m/s 60kg m/s20kg m/s
p =60kg m/sA
Second round
36
36
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37. (c) At the end of 5 round trip the linear momentum of
(ball + ‘A) system
,5 40 5 200 /Ap kg m s= × == × == × == × =
,5200 (40 4) Av= += += += +
,5
50
/
11Av m s====
(d) ‘A’ can catch the ball untill the velocity of ‘A’ is less
than 5 m/s. After 5 round when ‘A’ through the ball
i.e., 6th time the velocity of ‘A’ become greater than
5 m/s hence A can through the ball only 6 times.
(b) pA,1 = 40 = (40+4) vA,1
,1
40 10
/
44 11Av m s= == == == =
37
37
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38. Let the centre of mass is at a distance x cm from the
initial position of A.
(40 40 4) 40 0 4 0 40cmx d+ + = × + × ++ + = × + × ++ + = × + × ++ + = × + × +
10
21cmx m==== From initial position of A.
(e) As no external force is acting on ‘A’, ‘B’ and ‘ball’
system hence the position of centre of mass of
system should remain constant always.
38
38
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39. 39
Problem 41.Problem 41.
A block of mass 2.0 kg is moving on a frictionless
horizontal surface with a velocity of 1.0 m/s towards
another block of equal mass kept at rest. The spring
constant of the spring fixed at one end is 100 N/m.
Find the maximum compression of the spring .
1.0 m/s
2 kg 2 kg
39
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40. Problem 42.Problem 42.
A bullet of mass 20 g travelling horizontally with a speed
of 500 m/s passes through a wooden block of mass 10.
0 kg initially at rest on a level surface. The bullet
emerges with a speed of 100 m/s and the block slides
20 cm on the surface before coming to rest.
Find the friction coefficient between the block and the
surface.
40
500 m/s
40
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41. Problem 43.Problem 43.
A projectile is fired with a speed u at an angle θ above a
horizontal field. The coefficient of restitution of collision
between the projectile and the field is e.
How far from the starting point, does the projectile
makes its second collision with the field ?
41
41
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42. Problem 46.Problem 46.
A block of mass 200 g is suspended through a vertical
spring. The spring is stretched by 1.0 cm when the block
is in equilibrium. A particle of mass 120 g is dropped on
the block from a height of 45 cm. The particle sticks to
the block after the impact.
Find the maximum extension of the spring.
Take g = 10 m/s2.
42
p v
42
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43. Problem 49.Problem 49.
Two masses m1 and m2 are connected by a spring of
spring constant k and are placed on a frictionless
horizontal surface. Initially the spring is stretched
through a distance x0 when the system is released from
rest.
Find the distance moved by the two masses before they
again come to rest.
43
43
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44. Problem 50.Problem 50.
Two blocks of masses m1 and m2 are connected by a
spring of spring constant k. The block of mass m2 is
given a sharp impulse so that it acquires a velocity v0
towards right.
Find
(a) the velocity of the centre of mass,
(b) the maximum elongation that the spring will
suffer.
44
m1 m2
v0
44
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45. Problem 51.Problem 51.
Consider the situation of the previous problem. Suppose
each of the blocks is pulled by a constant force F instead
of any impulse.
Find the maximum elongation that the spring will suffer
and the distances moved by the two blocks in the
process.
45
45
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46. Problem 52.Problem 52.
Consider the situation of the previous problem. Suppose
the block of mass m1 is pulled by a constant force F1 and
the other block is pulled by a constant force F2.
Find the maximum elongation that the spring will
suffer.
46
46
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47. Problem 54.Problem 54.
The track shown in figure is frictionless. The block B of
mass 2m is lying at rest and the block A of mass m is
pushed along the track with some speed. The collision
between A and B is perfectly elastic.
With what velocity should the block A be started to get
the sleeping man awakened ?
47
A
B
h h
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48. Problem 55.Problem 55.
A bullet of mass 10 g moving horizontally at a speed of
50√7 m/s strikes a block of mass 490 g kept on a
frictionless track as shown in the figure. The bullet
remains inside the block and the system proceeds
towards the semicircular track of radius 0.2 m.
Where will the block strike the horizontal part after
leaving the semicircular track ?
48
0.2 m
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49. Problem 56.Problem 56.
Two balls having masses m and 2m are fastened to two
light strings of some length l. The other ends of the
strings are fixed at O. The strings are kept in the same
horizontal line and the system is released from rest. The
collision between the balls is elastic.
(a) Find the velocities of the balls rise after the collision ?
(b) How high will the balls rise after the collision ?
49
m 2m
1 0 1
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50. Problem 57.Problem 57.
A uniform chain of mass M and length L is held vertically
in such a way that its lower end just touches the
horizontal floor. The chain is released from rest in this
position. Any portion that strikes the floor comes to rest.
Assuming that the chain does not form a heap on the
floor, calculate the force exerted by it on the floor when
a length x has reached the floor.
50
50
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51. Problem 58.Problem 58.
The blocks shown in figure have equal masses. The
surface of A is smooth but that of B has a friction
coefficient of 0.10 with the floor. Block A is moving at a
speed of 10 m/s towards B which is kept at rest.
Find the distance travelled by B if
(a) the collision is perfectly elastic and
(b) the collision is perfectly inelastic.
Take g = 10 m/s2.
51
A
10 m/s
B
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52. Problem 59.Problem 59.
The friction coefficient between the horizontal surface
and each of the blocks shown in figure is 0.20. The
collision between the blocks is perfectly elastic.
Find the separation between the two blocks when they
come to rest
Take = g = 10 m/s2.
52
2 kg
10 m/s
2 kg
16 cm
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53. Problem 60.Problem 60.
A block of mass m is placed on a triangular block of
mass M, which in turn is placed on a horizontal surface
as shown in figure. Assuming frictionless surfaces find
the velocity of the triangular block when the smaller
block reaches the bottom end.
53
m
M
h
α
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54. Problem 61.Problem 61.
Figure shows a small body of mass m placed over n
larger mass M whose surface is horizontal near the
smaller mass and gradually curves to become vertical.
The smaller mass is pushed on the longer one at a
speed v and the system is left to itself. Assume that all
the surfaces are frictionless.
(a) Find the speed of the larger block when the smaller
block is sliding on the vertical part.
(b) Find the speed of the smaller mass when it breaks
off the larger mass at height h.
(c) Find the maximum height (from the ground) that the
smaller mass ascends.
(d) Show that the smaller mass will again land on the
bigger one.
54
54
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55. Find the distance traversed by the bigger block
during the time when the smaller block was in its
flight under gravity .
55
m
M
h
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56. Problem 62.Problem 62.
A small block of superdense material has a mass of 3 ×
1024 kg. It is situated at a height h (much smaller than
the earth’s radius) from where it falls on the earth’s
surface.
Find its speed when its height from the earth’s surface
has reduced to h/2. The mass of the earth is 6 × 1024
kg.
56
56
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57. Problem 63.Problem 63.
A body of mass m makes an elastic collision with another
identical body at rest. Show that if the collision is not
head- on, the bodies go at right angle to each other
after the collision.
57
57
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58. Problem 64.Problem 64.
A small particles travelling with a velocity v collides
elastically with a spherical body of equal mass and of
radius r initially kept at rest. The centre of this spherical
body is located a distance p(< r) away from the direction
of motion of the particle .
Find the final velocities of the two particles.
[Hint : the force acts along the normal to the sphere
through the contact. Treat the collision as one-
dimensional for this direction. In the tangential direction
no force acts and the velocities do not change]
58
v
rp
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