SlideShare a Scribd company logo
1 of 42
Chapter 4
Force and Motion
Younes Sina
Force may be defined as the cause of motion and deformation.
When a force is applied to an object, the object either moves or
changes shape or both. In most cases, it is not possible to detect
the deformation by naked eyes at the molecular or atomic level.
Deformation occurs no matter how small.
The formula ΣF = M.a is called
the "Newton's 2nd Law of Motion."
Example : An 850-kg car is accelerating at a rate of
2.4m/s2 to the right along a straight and horizontal
road where it experiences an overall frictional force of
1500N. Determine the force that its engine exerts.
M= 850 kg
a= 2.4m/s2
Ff =1500N
Solution:
If "to the right" is taken to be positive as usual, Fe is
positive, and Ff negative. Note that friction always
opposes the direction of pending motion. Applying
Newton's 2nd law:
ΣF = Ma
Fe - Ff = Ma
Fe - 1500N = (850kg)(2.4m/s2)
Fe = 1500N + 2040N = 3500N
Note that the 2040N must be rounded to 2 significant
figures and then added to the 1500N.
Example : A 2400-kg truck is moving at a constant speed of 15m/s on
a horizontal and straight road that offers an overall frictional force of
1800N. Calculate
(a) its acceleration
(b) the engine force
(c) the distance it travels in 35s
(d) its acceleration if it changes its speed to 25m/s in 8.0 seconds,
(e) the engine force in this case.
M= 2400 kg
v= 15 m/s
Ff =1800N
Solution:
(a) Since the truck's speed is initially constant; therefore
a1 = 0
(b) ΣF = M.a
Fe - Ff = M.a1
Fe - 1800N = (2400kg)(0)
Fe = 1800N + 0 = 1800N
(c) x = v t (Equation of motion for constant velocity)
x = (15m/s)(35s) = 530m (rounded to 2 sig. fig.)
(d) a2 = (Vf - Vi) / t
a2 = (25m/s - 15m/s) / 8.0s = 1.25 m/s2
(e) ΣF = M.a
Fe - Ff = M.a2
Fe - 1800N = (2400kg)(1.25m/s2)
Fe = 1800N + 3000N = 4800N
Example : A car that weighs 14700N is traveling along a straight road at a speed
of 108 km/h. The driver sees a deer on the road and has to bring the car to stop in
a distance of 90 m. Determine
(a) the necessary deceleration
(b) the stopping force
(c) the brakes force, if the road friction is 2100N,
(d) the stopping time
W=14700 N v=108 km/h
Ff = 2100N
x=90 m
Solution:
The mass of the car and its velocity in (m/s) must be determined first.
w = M. g → M = w/g
M = (14700N) / (9.8 m/s2)
M = 1500kg
Vi = (108 km/h ) (1000m / 1km) ( 1h / 3600s) = 30.m/s
(a) Vf
2 - Vi
2 = 2 a x → (0) 2 - (30.)2 = 2 (a) (90.0m)
-900 = 180a
a = - 5.0 m/s2 (deceleration)
(b) ΣF = Ma
ΣF = (1500kg)(- 5.0 m/s2 ) = -7500N
(c) ΣF = Fbrakes + Ffriction
-7500N = Fbrakes - 2100N
Fbrakes = - 5400N
(d) a = (Vf - Vi) / t
t = (Vf - Vi) / a
t = (0 - 30.m/s) / (-5.0m/s2)
t = 6.0 seconds
Example: A 20.0-kg crate is on a horizontal and frictionless surface
as shown.
(a) Calculate and show the vertical forces acting on this crate.
(b) Knowing that the crate is being pushed to the left by a
53-N force, what magnitude force (F) to the right must be applied
onto the block to give it an acceleration of 2.5m/s2 to the right?
W=20.0 kg F=53 N a=2.5 m/s2
F
Example : An 80.0-kg man is standing in an elevator. Determine
the force of the elevator onto the person if the elevator is
(a) accelerating upward at 2.5m/s2
(b) going upward at constant speed
(c) coming to stop going upward at a deceleration of 2.5m/s2
(d) going downward at an acceleration of 2.5m/s2.
Solution: The force of the elevator onto the person is nothing but the normal
reaction, N, of the floor onto his feet. For each case, a force diagram must be
drawn. Let's take the +y-axis to be upward.
(a) w = M.g = (80kg)(-9.8 m/s2) = -780N
This is the case that the elevator has just started going
upward. Since its speed has to change from zero to some value, it
has to accelerate upward and the person feels heavier because the
floor of the elevator exerts a normal reaction, N , onto the man that
is greater than his weight. This creates a nonzero net force and
therefore accelerates the person.
ΣF = M.a
N - Mg = M.a
N =M (g + a)
N =M (g + a) = (80.0kg)(9.8+2.5)m/s2 = 984N
(b) w = Mg = (80kg)(-9.8 m/s2) = -780N
In this case, since the elevator goes up at constant speed,
its acceleration is zero and so is the acceleration of the man.
Zero acceleration means zero net force acting on the man.
This requires ( N ) to be equal to ( w ) in magnitude.
ΣF = Ma ; N - Mg = Ma
a=0 →
N =M.g = (80kg)(9.8)m/s2 = 780N
(c) w = Mg = (80kg)(-9.8 m/s2) = -780N
In this case, the elevator is coming to stop in its going upward. In
other words, it decelerates as it goes upward. We all have this
experience that during such slowing down, we feel lighter. We
will notice that the magnitude of the normal reaction, N,
becomes less than that of w.
ΣF = Ma
N - Mg = Ma
N =M (g + a)
N =M (g + a) = (80kg)(9.8 - 2.5)m/s2 = 580N
(d) w = Mg = (80kg)(-9.8 m/s2) = -780N
When the elevator starts going downward, its speed changes from
zero to some value, and therefore it accelerates.
This time we use -2.5 m/s2 because the acceleration vector is
downward.
ΣF = Ma ; N - Mg = Ma ; N =M (g + a)
N =M (g + a) = (80kg)(9.8-2.5)m/s2 = 580N
Example : In the figure shown, determine the
acceleration of the system of blocks:
2)If the cord is broken, does free fall occur?1) Does free fall occur?
"Yes""No"
Solution: Block B is not free to fall and must pull block A in addition to
moving itself. The vertical forces on block A cancel each other, according to
the Newton's 3rd law. The force of gravity on block B is the cause of motion
while block A is on the horizontal surface. In fact, we are only interested to
find the acceleration of the system of blocks while A slides horizontally. Let's
summarize: (1) the force that causes motion is WB and (2) this force has to
move both masses (MA + MB). Since the system is connected, both blocks
move at the same acceleration (same magnitude).
We may write:
ΣF = Ma
wB = (MA + MB) a
29N = ( 5.0 kg + 3.0 kg) a
a = 3.6 m/s2
Example: Vehicles A and B are shown in nine different cases.
In each case, a statement is made on the left. Refer to the figure
in the middle and determine if the statement is true (T) or false (F).
1) MA = MB. If A is pushing B at constant velocity,
then F1 = F2.
T
2) MA = MB; If A is pushing B and accelerating,
then F1 >F2.
3) MA = MB; If A is pushing B and decelerating,
then F1 <F2.
F
F
F1=MA. a
F2=MB. a
4) MA > MB; If A is pushing B at constant velocity,
then F1 > F2.
5) MA > MB; If A is pushing B and accelerating,
then F1 > F2.
F
F
6) MA > MB; If A is pushing B and decelerating,
then F1 < F2.
7) MA < MB; If A is pushing B at constant velocity,
then F1 = F2.
F
T
8) MA < MB; If A is pushing B and accelerating,
then F1 > F2.
9) MA < MB; If A is pushing B and decelerating,
then F1 < F2.
F
F
Friction: Friction is the result of engagement of surface
irregularities between two surfaces in contact.
Coefficient of Kinetic Friction ( μk ) on a horizontal surface:
horizontally applied force (Fappl.)/weight of the object (w)
to slide the object at a constant velocity
Fappl. = Fk
w = N
Fk = μkN
Example : The coefficient of kinetic friction between a cement
block and a plank of wood is 0.38 The block has a mass of 15 kg
and is placed horizontally on the plank. Find the magnitude of the
horizontal force that can push the block to the right at a
constant velocity.
Example : In the figure shown, determine the magnitude of the
horizontal force to the right that can move the block at
(a) constant velocity
(b) at an acceleration of 3.0 m/s2.
Solution: (a)
W= Mg = (25kg)(9.8m/s2) = 245 N
N = 245 N ; Fk = μkN = (0. 26)(245N) = 64 N
ΣF = Ma ; F - 64 = (25)( 0 ) ; F = 64 N
Solution: (b)
ΣF = Ma ; F - 64 = (25)(3. 0) N ; F = 139 N
Coefficient of Static Friction ( μs ) : On a horizontal surface, the ratio of the
horizontally applied force (Fappl.) to an object to the weight of the object (w),
to bring the object onto the verge of slipping, is called the coefficient of
static friction. This is mathematically written as:
on the verge of slipping
N = w
Fappl. = Fs
Example : The coefficient of static friction between a cement block and a plank
of wood is 0.46. The block has a mass of 15 kg and is placed horizontally on the
plank. Find the magnitude of the horizontal force that can bring the block onto
the verge of slipping.
Friction Laws:
There are 5 laws for friction. The first 3 apply to the force of friction, and the
last 2 to the coefficient of friction.
1) Force of friction ( Ff ) is proportional to the coefficient of friction ( μ ) and the
normal force ( N ).
Fs = μsN
Fk = μkN
Note that:
μs > μk → Fs >Fk
It takes a greater force to bring an object onto the verge of slipping than pushing
it at a constant velocity.
2) Force of friction ( Ff ) is always tangent or parallel to the contacting surfaces.
3) Force of friction ( Ff ) always opposes the direction of pending motion.
4) Coefficient of friction ( μ ) depends on the materials of the contacting
surfaces.
5) Coefficient of friction ( μ ) depends on the smoothness of the contacting
surfaces.
Example : Two kids are sitting on the opposite sides of a 2.9 m long table and
sliding a 150-gram empty cup toward each other, back and forth. The game is
to give the cup the right initial velocity at one edge such that it comes to stop
exactly at the opposite edge as shown. The diameter of the cup is 10.0cm.
The coefficient of kinetic friction between the cup and the horizontal tabletop
is 0.12. Determine the necessary initial speed.
X= 2.9 mΦ= 10.0cm
μ= 0.12
Solution:
We need to use the kinetic equation, ΣF = Ma in order to solve for acceleration.
What are the forces acting on the cup after it is given an initial instant push?
The only acting force is the force of kinetic friction, Fk.
To find Fk , we need to know N , and consequently (w).
w = Mg
w = Mg = (0.15kg)(9.8 m/s2) = 1.47N
N = 1.47N
Fk = μkN
Fk = (0.12)( 1.47 N ) = 0.176 N
ΣF = Ma
- 0.176N = (0.150kg)(a)
a = -1.173 m/s2
Vf
2 - Vi
2 = 2 a x
02 - Vi
2 = 2 (-1.173 m/s2)(2.9m)
Vi = 2.6 m/s
Example : A truck that weighs 29,400N traveling at 72.0 km/h on a horizontal
and straight road skids to stop in 6.00s. Determine
(a) its deceleration
(b) the stopping force
(c) the kinetic coefficient of friction between its tires and the horizontally
straight road,
(d) the stopping distance.
V= 72.0 km/hW= 29,400N
t= 6.00 s
Solution:
(a) a = (Vf - Vi) / t
a = (0-20.0m/s) / (6.00s) = - 3.33 m/s2.
w = Mg
29,400N = M(9.8m/s2)
M = 3,000kg
(b) ΣF = Ma
0 - Fk = (3000kg)(- 3.33m/s2) = -10,000N
Fk = 10,000N
(c) Fk = μkN
10,000N = ( μk ) (29400N)
μk = (10,000N) / (29400N) = 0.40
(d) x = (1/2)a t2 + Vi t
x = (1/2)(-3.33m/s2)(6.00s)2 + (20.0m/s)(6.00s) = 60.0m
Vf
2 - Vi
2 = 2 a x
(0)2 - (20.0m/s)2 = 2(-3.33m/s2) x
x = 60.0m
Example : A 12-kg box is placed on a horizontal floor for which μs = 0.43
and μk = 0.33. Does a 57-N force, applied horizontally to this box, put it into
motion? If yes, will the motion be accelerated or at constant speed?
If accelerated, how far will it travel in 3.0s?
M= 12 kg
μs = 0.43
μk = 0.33
F= 57N
Solution: We know that Fs > Fk .
If Fs (the force of static friction) is less than 57-N, the horizontally applied force,
motion will occur. Let's calculate Fs.
w = Mg
w = (12kg)(9.8 m/s2) = 118N
N = 118N
Fs = μsN
Fs =(0.43)118N = 51N
Since Fs < 57N ; therefore, motion occurs.
Once motion occurs, μk takes over.
Fk = μkN
Fk = (0.33)(118N) = 39N
The motion will be accelerated because the net force is not zero.
ΣF = Ma
57N - 39N = (12kg)( a )
a = 1.5 m/s2
x = (1/2)a t2 + Vi t
x = (1/2)(1.5m/s2)(3.0s)2 + (0)(3.0s)
x = 6.8m
Example : In the figure shown, determine the magnitude
of force F that gives the block an acceleration of 1.75m/s2
on the horizontal surface to the right.
To solve for F and N, let's move these unknowns to the left of each equation
while moving the known values to the right sides.
1) N - Fsin30 = 147
N - 0.500 F = 147
2) -.021N + Fcos30 = 26.25
-0.21 N + 0.866 F = 26.25
Alternate Solution: Before rearranging, substitute for N from the 1st equation
into the 2nd one as shown:
Fcos(30) - 0.21(147 + Fsin30) = 26.25
now, there is only one unknown, F.
0.866F - 30.87 - 0.105F = 26.25
0.761F = 57.12
F = 75N
From the N equation
N = 147 + 75sin30
N = 190 N
Homework:
All problems in chapter 4

More Related Content

What's hot

free fall objects terminal velocity
free fall objects terminal velocityfree fall objects terminal velocity
free fall objects terminal velocityjamesadam2001
 
Transformations of functions
Transformations of functionsTransformations of functions
Transformations of functionsVictoria Ball
 
Chapter 2.1 ticker timer notes
Chapter 2.1 ticker timer notesChapter 2.1 ticker timer notes
Chapter 2.1 ticker timer notesRishwin Sinda
 
IGCSE PHYSICS: Equilibrium and Centre of Mass
IGCSE PHYSICS: Equilibrium and Centre of MassIGCSE PHYSICS: Equilibrium and Centre of Mass
IGCSE PHYSICS: Equilibrium and Centre of MassRozzie Jhana CamQue
 
Relative velocity
Relative velocityRelative velocity
Relative velocityindrasir
 
Kinematics of a particle
Kinematics of a particle Kinematics of a particle
Kinematics of a particle shaifulawie77
 
Chapter 3 dynamics
Chapter 3 dynamicsChapter 3 dynamics
Chapter 3 dynamicsFahad Asif
 
Integral Calculus
Integral CalculusIntegral Calculus
Integral Calculusitutor
 
Turning effects of forces physics presentation for 9th grade Physics students...
Turning effects of forces physics presentation for 9th grade Physics students...Turning effects of forces physics presentation for 9th grade Physics students...
Turning effects of forces physics presentation for 9th grade Physics students...Physics Amal Sweis
 
Ap physics 12_-_kinematics
Ap physics 12_-_kinematicsAp physics 12_-_kinematics
Ap physics 12_-_kinematicskampkorten
 
Relative Velocity by UK Physics
Relative Velocity by UK PhysicsRelative Velocity by UK Physics
Relative Velocity by UK PhysicsUdayKhanal
 
Functions for Grade 10
Functions for Grade 10Functions for Grade 10
Functions for Grade 10Boipelo Radebe
 
Classifying triangles Holt
Classifying triangles   HoltClassifying triangles   Holt
Classifying triangles Holtsaleem halabi
 

What's hot (20)

Linear motion present
Linear motion presentLinear motion present
Linear motion present
 
free fall objects terminal velocity
free fall objects terminal velocityfree fall objects terminal velocity
free fall objects terminal velocity
 
Transformations of functions
Transformations of functionsTransformations of functions
Transformations of functions
 
Chapter 2.1 ticker timer notes
Chapter 2.1 ticker timer notesChapter 2.1 ticker timer notes
Chapter 2.1 ticker timer notes
 
IGCSE PHYSICS: Equilibrium and Centre of Mass
IGCSE PHYSICS: Equilibrium and Centre of MassIGCSE PHYSICS: Equilibrium and Centre of Mass
IGCSE PHYSICS: Equilibrium and Centre of Mass
 
Relative velocity
Relative velocityRelative velocity
Relative velocity
 
Projectile motion
Projectile motionProjectile motion
Projectile motion
 
Static Equilibrium
Static EquilibriumStatic Equilibrium
Static Equilibrium
 
Kinematics of a particle
Kinematics of a particle Kinematics of a particle
Kinematics of a particle
 
Chapter 3 dynamics
Chapter 3 dynamicsChapter 3 dynamics
Chapter 3 dynamics
 
Graph transformations
Graph transformationsGraph transformations
Graph transformations
 
Integral Calculus
Integral CalculusIntegral Calculus
Integral Calculus
 
Turning effects of forces physics presentation for 9th grade Physics students...
Turning effects of forces physics presentation for 9th grade Physics students...Turning effects of forces physics presentation for 9th grade Physics students...
Turning effects of forces physics presentation for 9th grade Physics students...
 
Ap physics 12_-_kinematics
Ap physics 12_-_kinematicsAp physics 12_-_kinematics
Ap physics 12_-_kinematics
 
Relative Velocity by UK Physics
Relative Velocity by UK PhysicsRelative Velocity by UK Physics
Relative Velocity by UK Physics
 
Vectors and scalars
Vectors and scalarsVectors and scalars
Vectors and scalars
 
Functions for Grade 10
Functions for Grade 10Functions for Grade 10
Functions for Grade 10
 
Momentum
MomentumMomentum
Momentum
 
Classifying triangles Holt
Classifying triangles   HoltClassifying triangles   Holt
Classifying triangles Holt
 
Friction
FrictionFriction
Friction
 

Viewers also liked

Viewers also liked (12)

Chapter 12
Chapter 12Chapter 12
Chapter 12
 
Chapter 6
Chapter 6Chapter 6
Chapter 6
 
Chapter 11
Chapter 11Chapter 11
Chapter 11
 
Chapter 14
Chapter 14Chapter 14
Chapter 14
 
Chapter 7
Chapter 7Chapter 7
Chapter 7
 
Physics by Younes Sina
Physics by Younes SinaPhysics by Younes Sina
Physics by Younes Sina
 
Chapter 5
Chapter 5Chapter 5
Chapter 5
 
Chapter 9
Chapter 9Chapter 9
Chapter 9
 
Chapter 8
Chapter 8Chapter 8
Chapter 8
 
Moments
MomentsMoments
Moments
 
Engineering mechanics-question-and-answers-for-gate-ias
Engineering mechanics-question-and-answers-for-gate-iasEngineering mechanics-question-and-answers-for-gate-ias
Engineering mechanics-question-and-answers-for-gate-ias
 
Hibbeler chapter5
Hibbeler chapter5Hibbeler chapter5
Hibbeler chapter5
 

Similar to Chapter 4 (20)

Long 50slideschapter 5 motion notes [autosaved]
Long 50slideschapter 5 motion notes [autosaved]Long 50slideschapter 5 motion notes [autosaved]
Long 50slideschapter 5 motion notes [autosaved]
 
Linear momentum and its conservation by Victor R. Oribe
Linear momentum and its conservation by Victor R. OribeLinear momentum and its conservation by Victor R. Oribe
Linear momentum and its conservation by Victor R. Oribe
 
App of the 2nd law single body problems
App of the 2nd law single body problemsApp of the 2nd law single body problems
App of the 2nd law single body problems
 
static friction
static frictionstatic friction
static friction
 
Chapter 9
Chapter 9Chapter 9
Chapter 9
 
Newton's second law
Newton's second lawNewton's second law
Newton's second law
 
ClassExamples_LinearMomentum.pdf
ClassExamples_LinearMomentum.pdfClassExamples_LinearMomentum.pdf
ClassExamples_LinearMomentum.pdf
 
JC A Level H2 Physics Dynamics Notes
JC A Level H2 Physics Dynamics NotesJC A Level H2 Physics Dynamics Notes
JC A Level H2 Physics Dynamics Notes
 
Ap review total
Ap review totalAp review total
Ap review total
 
Chap9
Chap9Chap9
Chap9
 
Oscillation & Oscillatory Motion
Oscillation & Oscillatory MotionOscillation & Oscillatory Motion
Oscillation & Oscillatory Motion
 
Friction
FrictionFriction
Friction
 
Every Equation
Every EquationEvery Equation
Every Equation
 
Work power-energy
Work power-energyWork power-energy
Work power-energy
 
Uniform Circular Motion
Uniform Circular MotionUniform Circular Motion
Uniform Circular Motion
 
Power point slides for momentum, Impullse conservation of memntum
Power point slides for momentum, Impullse conservation of memntumPower point slides for momentum, Impullse conservation of memntum
Power point slides for momentum, Impullse conservation of memntum
 
PHYSICS KSSM FORM 4 (2.6 Force)
PHYSICS KSSM FORM 4 (2.6 Force)PHYSICS KSSM FORM 4 (2.6 Force)
PHYSICS KSSM FORM 4 (2.6 Force)
 
5299254.ppt
5299254.ppt5299254.ppt
5299254.ppt
 
Lecture09
Lecture09Lecture09
Lecture09
 
Lecture09
Lecture09Lecture09
Lecture09
 

More from Younes Sina

ICDIM 2012 presentation
ICDIM 2012 presentationICDIM 2012 presentation
ICDIM 2012 presentationYounes Sina
 
Phase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemPhase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemYounes Sina
 
Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Younes Sina
 
Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Younes Sina
 
توسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدتوسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدYounes Sina
 
Nuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesNuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesYounes Sina
 
Ion implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkIon implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkYounes Sina
 
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina
 
Younes Sina, Ion Channeling
 Younes Sina, Ion Channeling  Younes Sina, Ion Channeling
Younes Sina, Ion Channeling Younes Sina
 
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina
 
Younes Sina's presentation on Nuclear reaction analysis
Younes Sina's presentation on  Nuclear reaction analysisYounes Sina's presentation on  Nuclear reaction analysis
Younes Sina's presentation on Nuclear reaction analysisYounes Sina
 
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...Younes Sina
 
Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry  Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry Younes Sina
 
A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry  A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry Younes Sina
 
Ion Implantation
Ion Implantation Ion Implantation
Ion Implantation Younes Sina
 
Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Younes Sina
 

More from Younes Sina (20)

Chapter 3
Chapter 3Chapter 3
Chapter 3
 
Chapter 2
Chapter 2Chapter 2
Chapter 2
 
Chapter 1
Chapter 1Chapter 1
Chapter 1
 
ICDIM 2012 presentation
ICDIM 2012 presentationICDIM 2012 presentation
ICDIM 2012 presentation
 
Phase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemPhase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 System
 
Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3
 
Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)
 
توسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدتوسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصد
 
Nuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesNuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclides
 
Ion implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkIon implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utk
 
RBS
RBSRBS
RBS
 
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
 
Younes Sina, Ion Channeling
 Younes Sina, Ion Channeling  Younes Sina, Ion Channeling
Younes Sina, Ion Channeling
 
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
 
Younes Sina's presentation on Nuclear reaction analysis
Younes Sina's presentation on  Nuclear reaction analysisYounes Sina's presentation on  Nuclear reaction analysis
Younes Sina's presentation on Nuclear reaction analysis
 
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
 
Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry  Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry
 
A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry  A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry
 
Ion Implantation
Ion Implantation Ion Implantation
Ion Implantation
 
Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3
 

Recently uploaded

Call Girls Ahmedabad +917728919243 call me Independent Escort Service
Call Girls Ahmedabad +917728919243 call me Independent Escort ServiceCall Girls Ahmedabad +917728919243 call me Independent Escort Service
Call Girls Ahmedabad +917728919243 call me Independent Escort Serviceshivanisharma5244
 
COMPOSTING : types of compost, merits and demerits
COMPOSTING : types of compost, merits and demeritsCOMPOSTING : types of compost, merits and demerits
COMPOSTING : types of compost, merits and demeritsCherry
 
Cyathodium bryophyte: morphology, anatomy, reproduction etc.
Cyathodium bryophyte: morphology, anatomy, reproduction etc.Cyathodium bryophyte: morphology, anatomy, reproduction etc.
Cyathodium bryophyte: morphology, anatomy, reproduction etc.Cherry
 
The Mariana Trench remarkable geological features on Earth.pptx
The Mariana Trench remarkable geological features on Earth.pptxThe Mariana Trench remarkable geological features on Earth.pptx
The Mariana Trench remarkable geological features on Earth.pptxseri bangash
 
PODOCARPUS...........................pptx
PODOCARPUS...........................pptxPODOCARPUS...........................pptx
PODOCARPUS...........................pptxCherry
 
development of diagnostic enzyme assay to detect leuser virus
development of diagnostic enzyme assay to detect leuser virusdevelopment of diagnostic enzyme assay to detect leuser virus
development of diagnostic enzyme assay to detect leuser virusNazaninKarimi6
 
Factory Acceptance Test( FAT).pptx .
Factory Acceptance Test( FAT).pptx       .Factory Acceptance Test( FAT).pptx       .
Factory Acceptance Test( FAT).pptx .Poonam Aher Patil
 
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.Cherry
 
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryFAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryAlex Henderson
 
POGONATUM : morphology, anatomy, reproduction etc.
POGONATUM : morphology, anatomy, reproduction etc.POGONATUM : morphology, anatomy, reproduction etc.
POGONATUM : morphology, anatomy, reproduction etc.Cherry
 
Pteris : features, anatomy, morphology and lifecycle
Pteris : features, anatomy, morphology and lifecyclePteris : features, anatomy, morphology and lifecycle
Pteris : features, anatomy, morphology and lifecycleCherry
 
X-rays from a Central “Exhaust Vent” of the Galactic Center Chimney
X-rays from a Central “Exhaust Vent” of the Galactic Center ChimneyX-rays from a Central “Exhaust Vent” of the Galactic Center Chimney
X-rays from a Central “Exhaust Vent” of the Galactic Center ChimneySérgio Sacani
 
FS P2 COMBO MSTA LAST PUSH past exam papers.
FS P2 COMBO MSTA LAST PUSH past exam papers.FS P2 COMBO MSTA LAST PUSH past exam papers.
FS P2 COMBO MSTA LAST PUSH past exam papers.takadzanijustinmaime
 
Porella : features, morphology, anatomy, reproduction etc.
Porella : features, morphology, anatomy, reproduction etc.Porella : features, morphology, anatomy, reproduction etc.
Porella : features, morphology, anatomy, reproduction etc.Cherry
 
GBSN - Microbiology (Unit 3)Defense Mechanism of the body
GBSN - Microbiology (Unit 3)Defense Mechanism of the body GBSN - Microbiology (Unit 3)Defense Mechanism of the body
GBSN - Microbiology (Unit 3)Defense Mechanism of the body Areesha Ahmad
 
FAIRSpectra - Enabling the FAIRification of Analytical Science
FAIRSpectra - Enabling the FAIRification of Analytical ScienceFAIRSpectra - Enabling the FAIRification of Analytical Science
FAIRSpectra - Enabling the FAIRification of Analytical ScienceAlex Henderson
 
CYTOGENETIC MAP................ ppt.pptx
CYTOGENETIC MAP................ ppt.pptxCYTOGENETIC MAP................ ppt.pptx
CYTOGENETIC MAP................ ppt.pptxCherry
 

Recently uploaded (20)

Call Girls Ahmedabad +917728919243 call me Independent Escort Service
Call Girls Ahmedabad +917728919243 call me Independent Escort ServiceCall Girls Ahmedabad +917728919243 call me Independent Escort Service
Call Girls Ahmedabad +917728919243 call me Independent Escort Service
 
COMPOSTING : types of compost, merits and demerits
COMPOSTING : types of compost, merits and demeritsCOMPOSTING : types of compost, merits and demerits
COMPOSTING : types of compost, merits and demerits
 
Cyathodium bryophyte: morphology, anatomy, reproduction etc.
Cyathodium bryophyte: morphology, anatomy, reproduction etc.Cyathodium bryophyte: morphology, anatomy, reproduction etc.
Cyathodium bryophyte: morphology, anatomy, reproduction etc.
 
BHUBANESHWAR ODIA CALL GIRL SEIRVEC ❣️ 72051//37929❣️ CALL GIRL IN ODIA HAND ...
BHUBANESHWAR ODIA CALL GIRL SEIRVEC ❣️ 72051//37929❣️ CALL GIRL IN ODIA HAND ...BHUBANESHWAR ODIA CALL GIRL SEIRVEC ❣️ 72051//37929❣️ CALL GIRL IN ODIA HAND ...
BHUBANESHWAR ODIA CALL GIRL SEIRVEC ❣️ 72051//37929❣️ CALL GIRL IN ODIA HAND ...
 
The Mariana Trench remarkable geological features on Earth.pptx
The Mariana Trench remarkable geological features on Earth.pptxThe Mariana Trench remarkable geological features on Earth.pptx
The Mariana Trench remarkable geological features on Earth.pptx
 
PODOCARPUS...........................pptx
PODOCARPUS...........................pptxPODOCARPUS...........................pptx
PODOCARPUS...........................pptx
 
development of diagnostic enzyme assay to detect leuser virus
development of diagnostic enzyme assay to detect leuser virusdevelopment of diagnostic enzyme assay to detect leuser virus
development of diagnostic enzyme assay to detect leuser virus
 
Factory Acceptance Test( FAT).pptx .
Factory Acceptance Test( FAT).pptx       .Factory Acceptance Test( FAT).pptx       .
Factory Acceptance Test( FAT).pptx .
 
PATNA CALL GIRLS 8617370543 LOW PRICE ESCORT SERVICE
PATNA CALL GIRLS 8617370543 LOW PRICE ESCORT SERVICEPATNA CALL GIRLS 8617370543 LOW PRICE ESCORT SERVICE
PATNA CALL GIRLS 8617370543 LOW PRICE ESCORT SERVICE
 
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.
Genome Projects : Human, Rice,Wheat,E coli and Arabidopsis.
 
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryFAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
 
POGONATUM : morphology, anatomy, reproduction etc.
POGONATUM : morphology, anatomy, reproduction etc.POGONATUM : morphology, anatomy, reproduction etc.
POGONATUM : morphology, anatomy, reproduction etc.
 
Pteris : features, anatomy, morphology and lifecycle
Pteris : features, anatomy, morphology and lifecyclePteris : features, anatomy, morphology and lifecycle
Pteris : features, anatomy, morphology and lifecycle
 
X-rays from a Central “Exhaust Vent” of the Galactic Center Chimney
X-rays from a Central “Exhaust Vent” of the Galactic Center ChimneyX-rays from a Central “Exhaust Vent” of the Galactic Center Chimney
X-rays from a Central “Exhaust Vent” of the Galactic Center Chimney
 
FS P2 COMBO MSTA LAST PUSH past exam papers.
FS P2 COMBO MSTA LAST PUSH past exam papers.FS P2 COMBO MSTA LAST PUSH past exam papers.
FS P2 COMBO MSTA LAST PUSH past exam papers.
 
Porella : features, morphology, anatomy, reproduction etc.
Porella : features, morphology, anatomy, reproduction etc.Porella : features, morphology, anatomy, reproduction etc.
Porella : features, morphology, anatomy, reproduction etc.
 
GBSN - Microbiology (Unit 3)Defense Mechanism of the body
GBSN - Microbiology (Unit 3)Defense Mechanism of the body GBSN - Microbiology (Unit 3)Defense Mechanism of the body
GBSN - Microbiology (Unit 3)Defense Mechanism of the body
 
ABHISHEK ANTIBIOTICS PPT MICROBIOLOGY // USES OF ANTIOBIOTICS TYPES OF ANTIB...
ABHISHEK ANTIBIOTICS PPT MICROBIOLOGY  // USES OF ANTIOBIOTICS TYPES OF ANTIB...ABHISHEK ANTIBIOTICS PPT MICROBIOLOGY  // USES OF ANTIOBIOTICS TYPES OF ANTIB...
ABHISHEK ANTIBIOTICS PPT MICROBIOLOGY // USES OF ANTIOBIOTICS TYPES OF ANTIB...
 
FAIRSpectra - Enabling the FAIRification of Analytical Science
FAIRSpectra - Enabling the FAIRification of Analytical ScienceFAIRSpectra - Enabling the FAIRification of Analytical Science
FAIRSpectra - Enabling the FAIRification of Analytical Science
 
CYTOGENETIC MAP................ ppt.pptx
CYTOGENETIC MAP................ ppt.pptxCYTOGENETIC MAP................ ppt.pptx
CYTOGENETIC MAP................ ppt.pptx
 

Chapter 4

  • 1. Chapter 4 Force and Motion Younes Sina
  • 2. Force may be defined as the cause of motion and deformation. When a force is applied to an object, the object either moves or changes shape or both. In most cases, it is not possible to detect the deformation by naked eyes at the molecular or atomic level. Deformation occurs no matter how small.
  • 3. The formula ΣF = M.a is called the "Newton's 2nd Law of Motion."
  • 4. Example : An 850-kg car is accelerating at a rate of 2.4m/s2 to the right along a straight and horizontal road where it experiences an overall frictional force of 1500N. Determine the force that its engine exerts. M= 850 kg a= 2.4m/s2 Ff =1500N
  • 5. Solution: If "to the right" is taken to be positive as usual, Fe is positive, and Ff negative. Note that friction always opposes the direction of pending motion. Applying Newton's 2nd law: ΣF = Ma Fe - Ff = Ma Fe - 1500N = (850kg)(2.4m/s2) Fe = 1500N + 2040N = 3500N Note that the 2040N must be rounded to 2 significant figures and then added to the 1500N.
  • 6. Example : A 2400-kg truck is moving at a constant speed of 15m/s on a horizontal and straight road that offers an overall frictional force of 1800N. Calculate (a) its acceleration (b) the engine force (c) the distance it travels in 35s (d) its acceleration if it changes its speed to 25m/s in 8.0 seconds, (e) the engine force in this case. M= 2400 kg v= 15 m/s Ff =1800N
  • 7. Solution: (a) Since the truck's speed is initially constant; therefore a1 = 0 (b) ΣF = M.a Fe - Ff = M.a1 Fe - 1800N = (2400kg)(0) Fe = 1800N + 0 = 1800N (c) x = v t (Equation of motion for constant velocity) x = (15m/s)(35s) = 530m (rounded to 2 sig. fig.) (d) a2 = (Vf - Vi) / t a2 = (25m/s - 15m/s) / 8.0s = 1.25 m/s2 (e) ΣF = M.a Fe - Ff = M.a2 Fe - 1800N = (2400kg)(1.25m/s2) Fe = 1800N + 3000N = 4800N
  • 8. Example : A car that weighs 14700N is traveling along a straight road at a speed of 108 km/h. The driver sees a deer on the road and has to bring the car to stop in a distance of 90 m. Determine (a) the necessary deceleration (b) the stopping force (c) the brakes force, if the road friction is 2100N, (d) the stopping time W=14700 N v=108 km/h Ff = 2100N x=90 m
  • 9. Solution: The mass of the car and its velocity in (m/s) must be determined first. w = M. g → M = w/g M = (14700N) / (9.8 m/s2) M = 1500kg Vi = (108 km/h ) (1000m / 1km) ( 1h / 3600s) = 30.m/s (a) Vf 2 - Vi 2 = 2 a x → (0) 2 - (30.)2 = 2 (a) (90.0m) -900 = 180a a = - 5.0 m/s2 (deceleration) (b) ΣF = Ma ΣF = (1500kg)(- 5.0 m/s2 ) = -7500N (c) ΣF = Fbrakes + Ffriction -7500N = Fbrakes - 2100N Fbrakes = - 5400N (d) a = (Vf - Vi) / t t = (Vf - Vi) / a t = (0 - 30.m/s) / (-5.0m/s2) t = 6.0 seconds
  • 10. Example: A 20.0-kg crate is on a horizontal and frictionless surface as shown. (a) Calculate and show the vertical forces acting on this crate. (b) Knowing that the crate is being pushed to the left by a 53-N force, what magnitude force (F) to the right must be applied onto the block to give it an acceleration of 2.5m/s2 to the right? W=20.0 kg F=53 N a=2.5 m/s2 F
  • 11.
  • 12. Example : An 80.0-kg man is standing in an elevator. Determine the force of the elevator onto the person if the elevator is (a) accelerating upward at 2.5m/s2 (b) going upward at constant speed (c) coming to stop going upward at a deceleration of 2.5m/s2 (d) going downward at an acceleration of 2.5m/s2.
  • 13. Solution: The force of the elevator onto the person is nothing but the normal reaction, N, of the floor onto his feet. For each case, a force diagram must be drawn. Let's take the +y-axis to be upward. (a) w = M.g = (80kg)(-9.8 m/s2) = -780N This is the case that the elevator has just started going upward. Since its speed has to change from zero to some value, it has to accelerate upward and the person feels heavier because the floor of the elevator exerts a normal reaction, N , onto the man that is greater than his weight. This creates a nonzero net force and therefore accelerates the person. ΣF = M.a N - Mg = M.a N =M (g + a) N =M (g + a) = (80.0kg)(9.8+2.5)m/s2 = 984N
  • 14. (b) w = Mg = (80kg)(-9.8 m/s2) = -780N In this case, since the elevator goes up at constant speed, its acceleration is zero and so is the acceleration of the man. Zero acceleration means zero net force acting on the man. This requires ( N ) to be equal to ( w ) in magnitude. ΣF = Ma ; N - Mg = Ma a=0 → N =M.g = (80kg)(9.8)m/s2 = 780N
  • 15. (c) w = Mg = (80kg)(-9.8 m/s2) = -780N In this case, the elevator is coming to stop in its going upward. In other words, it decelerates as it goes upward. We all have this experience that during such slowing down, we feel lighter. We will notice that the magnitude of the normal reaction, N, becomes less than that of w. ΣF = Ma N - Mg = Ma N =M (g + a) N =M (g + a) = (80kg)(9.8 - 2.5)m/s2 = 580N
  • 16. (d) w = Mg = (80kg)(-9.8 m/s2) = -780N When the elevator starts going downward, its speed changes from zero to some value, and therefore it accelerates. This time we use -2.5 m/s2 because the acceleration vector is downward. ΣF = Ma ; N - Mg = Ma ; N =M (g + a) N =M (g + a) = (80kg)(9.8-2.5)m/s2 = 580N
  • 17. Example : In the figure shown, determine the acceleration of the system of blocks: 2)If the cord is broken, does free fall occur?1) Does free fall occur? "Yes""No"
  • 18. Solution: Block B is not free to fall and must pull block A in addition to moving itself. The vertical forces on block A cancel each other, according to the Newton's 3rd law. The force of gravity on block B is the cause of motion while block A is on the horizontal surface. In fact, we are only interested to find the acceleration of the system of blocks while A slides horizontally. Let's summarize: (1) the force that causes motion is WB and (2) this force has to move both masses (MA + MB). Since the system is connected, both blocks move at the same acceleration (same magnitude). We may write: ΣF = Ma wB = (MA + MB) a 29N = ( 5.0 kg + 3.0 kg) a a = 3.6 m/s2
  • 19. Example: Vehicles A and B are shown in nine different cases. In each case, a statement is made on the left. Refer to the figure in the middle and determine if the statement is true (T) or false (F). 1) MA = MB. If A is pushing B at constant velocity, then F1 = F2. T
  • 20. 2) MA = MB; If A is pushing B and accelerating, then F1 >F2. 3) MA = MB; If A is pushing B and decelerating, then F1 <F2. F F F1=MA. a F2=MB. a
  • 21. 4) MA > MB; If A is pushing B at constant velocity, then F1 > F2. 5) MA > MB; If A is pushing B and accelerating, then F1 > F2. F F
  • 22. 6) MA > MB; If A is pushing B and decelerating, then F1 < F2. 7) MA < MB; If A is pushing B at constant velocity, then F1 = F2. F T
  • 23. 8) MA < MB; If A is pushing B and accelerating, then F1 > F2. 9) MA < MB; If A is pushing B and decelerating, then F1 < F2. F F
  • 24. Friction: Friction is the result of engagement of surface irregularities between two surfaces in contact. Coefficient of Kinetic Friction ( μk ) on a horizontal surface: horizontally applied force (Fappl.)/weight of the object (w) to slide the object at a constant velocity Fappl. = Fk w = N
  • 26. Example : The coefficient of kinetic friction between a cement block and a plank of wood is 0.38 The block has a mass of 15 kg and is placed horizontally on the plank. Find the magnitude of the horizontal force that can push the block to the right at a constant velocity.
  • 27.
  • 28. Example : In the figure shown, determine the magnitude of the horizontal force to the right that can move the block at (a) constant velocity (b) at an acceleration of 3.0 m/s2. Solution: (a) W= Mg = (25kg)(9.8m/s2) = 245 N N = 245 N ; Fk = μkN = (0. 26)(245N) = 64 N ΣF = Ma ; F - 64 = (25)( 0 ) ; F = 64 N Solution: (b) ΣF = Ma ; F - 64 = (25)(3. 0) N ; F = 139 N
  • 29. Coefficient of Static Friction ( μs ) : On a horizontal surface, the ratio of the horizontally applied force (Fappl.) to an object to the weight of the object (w), to bring the object onto the verge of slipping, is called the coefficient of static friction. This is mathematically written as: on the verge of slipping N = w Fappl. = Fs
  • 30. Example : The coefficient of static friction between a cement block and a plank of wood is 0.46. The block has a mass of 15 kg and is placed horizontally on the plank. Find the magnitude of the horizontal force that can bring the block onto the verge of slipping.
  • 31.
  • 32. Friction Laws: There are 5 laws for friction. The first 3 apply to the force of friction, and the last 2 to the coefficient of friction. 1) Force of friction ( Ff ) is proportional to the coefficient of friction ( μ ) and the normal force ( N ). Fs = μsN Fk = μkN Note that: μs > μk → Fs >Fk It takes a greater force to bring an object onto the verge of slipping than pushing it at a constant velocity. 2) Force of friction ( Ff ) is always tangent or parallel to the contacting surfaces. 3) Force of friction ( Ff ) always opposes the direction of pending motion. 4) Coefficient of friction ( μ ) depends on the materials of the contacting surfaces. 5) Coefficient of friction ( μ ) depends on the smoothness of the contacting surfaces.
  • 33. Example : Two kids are sitting on the opposite sides of a 2.9 m long table and sliding a 150-gram empty cup toward each other, back and forth. The game is to give the cup the right initial velocity at one edge such that it comes to stop exactly at the opposite edge as shown. The diameter of the cup is 10.0cm. The coefficient of kinetic friction between the cup and the horizontal tabletop is 0.12. Determine the necessary initial speed. X= 2.9 mΦ= 10.0cm μ= 0.12
  • 34. Solution: We need to use the kinetic equation, ΣF = Ma in order to solve for acceleration. What are the forces acting on the cup after it is given an initial instant push? The only acting force is the force of kinetic friction, Fk. To find Fk , we need to know N , and consequently (w). w = Mg w = Mg = (0.15kg)(9.8 m/s2) = 1.47N N = 1.47N Fk = μkN Fk = (0.12)( 1.47 N ) = 0.176 N ΣF = Ma - 0.176N = (0.150kg)(a) a = -1.173 m/s2 Vf 2 - Vi 2 = 2 a x 02 - Vi 2 = 2 (-1.173 m/s2)(2.9m) Vi = 2.6 m/s
  • 35. Example : A truck that weighs 29,400N traveling at 72.0 km/h on a horizontal and straight road skids to stop in 6.00s. Determine (a) its deceleration (b) the stopping force (c) the kinetic coefficient of friction between its tires and the horizontally straight road, (d) the stopping distance. V= 72.0 km/hW= 29,400N t= 6.00 s
  • 36. Solution: (a) a = (Vf - Vi) / t a = (0-20.0m/s) / (6.00s) = - 3.33 m/s2. w = Mg 29,400N = M(9.8m/s2) M = 3,000kg (b) ΣF = Ma 0 - Fk = (3000kg)(- 3.33m/s2) = -10,000N Fk = 10,000N (c) Fk = μkN 10,000N = ( μk ) (29400N) μk = (10,000N) / (29400N) = 0.40 (d) x = (1/2)a t2 + Vi t x = (1/2)(-3.33m/s2)(6.00s)2 + (20.0m/s)(6.00s) = 60.0m Vf 2 - Vi 2 = 2 a x (0)2 - (20.0m/s)2 = 2(-3.33m/s2) x x = 60.0m
  • 37. Example : A 12-kg box is placed on a horizontal floor for which μs = 0.43 and μk = 0.33. Does a 57-N force, applied horizontally to this box, put it into motion? If yes, will the motion be accelerated or at constant speed? If accelerated, how far will it travel in 3.0s? M= 12 kg μs = 0.43 μk = 0.33 F= 57N
  • 38. Solution: We know that Fs > Fk . If Fs (the force of static friction) is less than 57-N, the horizontally applied force, motion will occur. Let's calculate Fs. w = Mg w = (12kg)(9.8 m/s2) = 118N N = 118N Fs = μsN Fs =(0.43)118N = 51N Since Fs < 57N ; therefore, motion occurs. Once motion occurs, μk takes over. Fk = μkN Fk = (0.33)(118N) = 39N The motion will be accelerated because the net force is not zero. ΣF = Ma 57N - 39N = (12kg)( a ) a = 1.5 m/s2 x = (1/2)a t2 + Vi t x = (1/2)(1.5m/s2)(3.0s)2 + (0)(3.0s) x = 6.8m
  • 39. Example : In the figure shown, determine the magnitude of force F that gives the block an acceleration of 1.75m/s2 on the horizontal surface to the right.
  • 40.
  • 41. To solve for F and N, let's move these unknowns to the left of each equation while moving the known values to the right sides. 1) N - Fsin30 = 147 N - 0.500 F = 147 2) -.021N + Fcos30 = 26.25 -0.21 N + 0.866 F = 26.25 Alternate Solution: Before rearranging, substitute for N from the 1st equation into the 2nd one as shown: Fcos(30) - 0.21(147 + Fsin30) = 26.25 now, there is only one unknown, F. 0.866F - 30.87 - 0.105F = 26.25 0.761F = 57.12 F = 75N From the N equation N = 147 + 75sin30 N = 190 N