SlideShare a Scribd company logo
1 of 13
F E B R U A R Y 2 6 , 2 0 1 4
KINETICS AND PARTICLES:
FORCE and ACCELERATION
2 Main Factors that affect motion
in an Object
1. The Forces acting on an object
2. The Mass of an object
Mass – amount of matter in an object
- property of an object that specifies how
much resistance an object exhibits to
change in velocity
Acceleration – is the rate of change of the
velocity
Force – push or pull of an Object
– according to Isaac Newton, these are
what causes any change in the
velocity of an object at the same
time, it causes acceleration.
Newton's Laws
Newton described force as the ability to cause a mass to
accelerate.
First law: When the sum of the forces acting on a particle is
zero, its velocity is constant. In particular, if the particle is
initially stationary, it will remain stationary. Or if it moves
with constant speed in a single direction.
Second law: The rate of change of linear momentum of an
object is directly proportional to the applied force F and the
object moves in the direction in which force F is applied. If
the mass is constant, the sum of the forces is equal to the
product of the mass of the particle and its acceleration.
F = ma
Newton's Laws
Third law: The forces exerted by two particles on each other
are equal in magnitude and opposite in direction.
F2 = −F1
4th Law : Newton’s Gravitational Attraction
This law governs the gravitational attraction between
any two particles/bodies.
Newton's 2nd Law of Motion
The force and acceleration are directly
proportional, the constant of proportionality can be
determined in the ratio m = F1 / a1,
on the other hand if another force of different magnitude
say, (F2) is acted on an object, it will create another
acceleration say, a2 such that m = F2 / a2…
Thus, m serves as the constant of proportionality.
Equation of Motion
F = ma
In the case that 2 or more forces acting on a particle, the
resultant force is determined by a vector summation of all
the forces.
FR = F
Generally, the equation of motion is written as
F = ma
Static Equilibrium:
F = 0 FR = F = 0 thus , a = 0
Dynamic Equilibrium:
FR = F = ma F – ma = 0
Equations of Motion: Rectangular Coordinates
In a x,y & z frame of reference,
the forces acting on a particle can be expressed in
terms of i, j, k components, so we have
F = ma
Fx i + Fy j + Fz k = m ( ax i + ay j + az k )
To satisfy the given condition with its respective
i, j, k components:
Fx = max Fy = may Fz = maz
F R I CT I O N :
If the particle contacts on rough surface,
it is necessary to use the frictional equation, which relates
the coefficient of Kinetic Friction µk to the magnitude of
the Frictional Force (Ff) and Normal Force (N) acting on
the surface of contact,
Ff = µk N
Where: Ff - frictional force acting opposite
the subjected Force
µk - coefficient of kinetic friction
N - normal force
- force acting perpendicular to the point of
contact.
The 50 kg crate rests on a horizontal plane for which the
coefficient of kinetic friction is µk = 0.3 . If the crate is
subjected to a 400-N towing force 30⁰ from the horizontal,
determine the velocity of the crate in 5 sec starting from
rest.
EXAMPLE # 1
The 100 kg block A is released from rest. If the
mass of the pulleys and the cord are neglected,
determine the speed of the 20 kg block B in 2
seconds.
EXAMPLE # 2
At a given instant the 10 kg block A is moving downward
with a speed of 6 m/s. determine its speed 2 sec later.
Block B has a weight of 4 kg, and the coefficient of kinetic
friction between it and the horizontal plane is µk = 0.2 .
Neglect the mass of the pulleys and cord.
EXAMPLE # 3
Determine the time needed to pull the cord at B down 4 m
starting from rest when a force of 10 kg is applied to the
cord. Block A weighs 20 kg. Neglect the mass of the
pulleys and cords.
EXAMPLE # 4

More Related Content

What's hot

moments couples and force couple systems by ahmad khan
moments couples and force couple systems by ahmad khanmoments couples and force couple systems by ahmad khan
moments couples and force couple systems by ahmad khanSelf-employed
 
Chapter 12 kinematics_of_a_particle
Chapter 12 kinematics_of_a_particleChapter 12 kinematics_of_a_particle
Chapter 12 kinematics_of_a_particleSelf-employed
 
Relative velocity
Relative velocityRelative velocity
Relative velocityindrasir
 
Damped Vibration In harmonic oscilation
Damped Vibration In harmonic oscilationDamped Vibration In harmonic oscilation
Damped Vibration In harmonic oscilationSaurav Roy
 
Support reactions
Support reactionsSupport reactions
Support reactionsKarnav Rana
 
Dynamics
DynamicsDynamics
Dynamicsnlahoud
 
9. kinematics of particles
9. kinematics of particles9. kinematics of particles
9. kinematics of particlesEkeeda
 
Moment of inertia
Moment of inertiaMoment of inertia
Moment of inertiaUsman Sajid
 
Normal stress & Shear Stress
 Normal stress & Shear Stress Normal stress & Shear Stress
Normal stress & Shear StressMESHAL ALMUTAIRI
 
Dynamics13lecture
Dynamics13lectureDynamics13lecture
Dynamics13lectureAbdou Secka
 
engineering statics: distributed forces-1
engineering statics: distributed forces-1engineering statics: distributed forces-1
engineering statics: distributed forces-1musadoto
 
Application Of Impulse Momentum Equation
Application Of Impulse Momentum Equation Application Of Impulse Momentum Equation
Application Of Impulse Momentum Equation Muhammad Usama Nawab
 

What's hot (20)

moments couples and force couple systems by ahmad khan
moments couples and force couple systems by ahmad khanmoments couples and force couple systems by ahmad khan
moments couples and force couple systems by ahmad khan
 
Chapter 12 kinematics_of_a_particle
Chapter 12 kinematics_of_a_particleChapter 12 kinematics_of_a_particle
Chapter 12 kinematics_of_a_particle
 
Rectilinear motion
Rectilinear motionRectilinear motion
Rectilinear motion
 
Relative velocity
Relative velocityRelative velocity
Relative velocity
 
TORSION (MECHANICS OF SOLIDS)
TORSION (MECHANICS OF SOLIDS)TORSION (MECHANICS OF SOLIDS)
TORSION (MECHANICS OF SOLIDS)
 
Statics
StaticsStatics
Statics
 
Damped Vibration In harmonic oscilation
Damped Vibration In harmonic oscilationDamped Vibration In harmonic oscilation
Damped Vibration In harmonic oscilation
 
Support reactions
Support reactionsSupport reactions
Support reactions
 
Impact of Free Jets
Impact of Free JetsImpact of Free Jets
Impact of Free Jets
 
statics
staticsstatics
statics
 
Dynamics
DynamicsDynamics
Dynamics
 
9. kinematics of particles
9. kinematics of particles9. kinematics of particles
9. kinematics of particles
 
Moment of inertia
Moment of inertiaMoment of inertia
Moment of inertia
 
Resultant of forces
Resultant of forcesResultant of forces
Resultant of forces
 
Normal stress & Shear Stress
 Normal stress & Shear Stress Normal stress & Shear Stress
Normal stress & Shear Stress
 
Dynamics13lecture
Dynamics13lectureDynamics13lecture
Dynamics13lecture
 
engineering statics: distributed forces-1
engineering statics: distributed forces-1engineering statics: distributed forces-1
engineering statics: distributed forces-1
 
Moment of inertia
Moment of inertia Moment of inertia
Moment of inertia
 
Introduction to Engineering Mechanics
Introduction to Engineering MechanicsIntroduction to Engineering Mechanics
Introduction to Engineering Mechanics
 
Application Of Impulse Momentum Equation
Application Of Impulse Momentum Equation Application Of Impulse Momentum Equation
Application Of Impulse Momentum Equation
 

Similar to Kinematics of particles

Newton laws of motion summer 17
Newton laws of motion summer 17Newton laws of motion summer 17
Newton laws of motion summer 17ABIR A HAPZU
 
Topic 3 - Newtons Laws L1 (1).pdf
Topic 3 - Newtons Laws L1 (1).pdfTopic 3 - Newtons Laws L1 (1).pdf
Topic 3 - Newtons Laws L1 (1).pdfmahamoh6
 
Chapter 4-powerpoint-1221714072609324-8
Chapter 4-powerpoint-1221714072609324-8Chapter 4-powerpoint-1221714072609324-8
Chapter 4-powerpoint-1221714072609324-8Cleophas Rwemera
 
Forces physics
Forces physicsForces physics
Forces physicsYashumb
 
Force_Lesson_Ch4.pdf
Force_Lesson_Ch4.pdfForce_Lesson_Ch4.pdf
Force_Lesson_Ch4.pdfMervatMarji2
 
Unit 5 mm9400 ver1.1(2014)
Unit 5 mm9400 ver1.1(2014)Unit 5 mm9400 ver1.1(2014)
Unit 5 mm9400 ver1.1(2014)all_engineering
 
3 equilibrium of concurrent forces and
3 equilibrium  of  concurrent  forces   and3 equilibrium  of  concurrent  forces   and
3 equilibrium of concurrent forces andfelna00
 
Newton’s Laws Of Motion
Newton’s Laws Of MotionNewton’s Laws Of Motion
Newton’s Laws Of Motioneliseb
 
Laws of Motion.pptx
Laws of Motion.pptxLaws of Motion.pptx
Laws of Motion.pptxtufgvj
 
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF Download
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF DownloadForce & Laws of Motion Class 9 Science Chapter- NCERT PDF Download
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF DownloadVivekanand Anglo Vedic Academy
 
Lecture Ch 04
Lecture Ch 04Lecture Ch 04
Lecture Ch 04rtrujill
 
008 newton's second law of motion
008 newton's second law of motion008 newton's second law of motion
008 newton's second law of motionphysics101
 

Similar to Kinematics of particles (20)

4_Forces.doc
4_Forces.doc4_Forces.doc
4_Forces.doc
 
Newton laws of motion summer 17
Newton laws of motion summer 17Newton laws of motion summer 17
Newton laws of motion summer 17
 
Force and laws of motion
Force and laws of motionForce and laws of motion
Force and laws of motion
 
Mechanics 1
Mechanics 1Mechanics 1
Mechanics 1
 
Topic 3 - Newtons Laws L1 (1).pdf
Topic 3 - Newtons Laws L1 (1).pdfTopic 3 - Newtons Laws L1 (1).pdf
Topic 3 - Newtons Laws L1 (1).pdf
 
Chapter 4-powerpoint-1221714072609324-8
Chapter 4-powerpoint-1221714072609324-8Chapter 4-powerpoint-1221714072609324-8
Chapter 4-powerpoint-1221714072609324-8
 
UNIT-V.pptx
UNIT-V.pptxUNIT-V.pptx
UNIT-V.pptx
 
Forces physics
Forces physicsForces physics
Forces physics
 
Force_Lesson_Ch4.pdf
Force_Lesson_Ch4.pdfForce_Lesson_Ch4.pdf
Force_Lesson_Ch4.pdf
 
Unit 5 mm9400 ver1.1(2014)
Unit 5 mm9400 ver1.1(2014)Unit 5 mm9400 ver1.1(2014)
Unit 5 mm9400 ver1.1(2014)
 
3 equilibrium of concurrent forces and
3 equilibrium  of  concurrent  forces   and3 equilibrium  of  concurrent  forces   and
3 equilibrium of concurrent forces and
 
Newton’s Laws Of Motion
Newton’s Laws Of MotionNewton’s Laws Of Motion
Newton’s Laws Of Motion
 
Md zakaria 2
Md zakaria 2Md zakaria 2
Md zakaria 2
 
Ch_04b.ppt
Ch_04b.pptCh_04b.ppt
Ch_04b.ppt
 
Newtons laws
Newtons lawsNewtons laws
Newtons laws
 
Laws of Motion.pptx
Laws of Motion.pptxLaws of Motion.pptx
Laws of Motion.pptx
 
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF Download
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF DownloadForce & Laws of Motion Class 9 Science Chapter- NCERT PDF Download
Force & Laws of Motion Class 9 Science Chapter- NCERT PDF Download
 
2.2 forces and dynamics
2.2   forces and dynamics2.2   forces and dynamics
2.2 forces and dynamics
 
Lecture Ch 04
Lecture Ch 04Lecture Ch 04
Lecture Ch 04
 
008 newton's second law of motion
008 newton's second law of motion008 newton's second law of motion
008 newton's second law of motion
 

Kinematics of particles

  • 1. F E B R U A R Y 2 6 , 2 0 1 4 KINETICS AND PARTICLES: FORCE and ACCELERATION
  • 2. 2 Main Factors that affect motion in an Object 1. The Forces acting on an object 2. The Mass of an object
  • 3. Mass – amount of matter in an object - property of an object that specifies how much resistance an object exhibits to change in velocity Acceleration – is the rate of change of the velocity Force – push or pull of an Object – according to Isaac Newton, these are what causes any change in the velocity of an object at the same time, it causes acceleration.
  • 4. Newton's Laws Newton described force as the ability to cause a mass to accelerate. First law: When the sum of the forces acting on a particle is zero, its velocity is constant. In particular, if the particle is initially stationary, it will remain stationary. Or if it moves with constant speed in a single direction. Second law: The rate of change of linear momentum of an object is directly proportional to the applied force F and the object moves in the direction in which force F is applied. If the mass is constant, the sum of the forces is equal to the product of the mass of the particle and its acceleration. F = ma
  • 5. Newton's Laws Third law: The forces exerted by two particles on each other are equal in magnitude and opposite in direction. F2 = −F1 4th Law : Newton’s Gravitational Attraction This law governs the gravitational attraction between any two particles/bodies.
  • 6. Newton's 2nd Law of Motion The force and acceleration are directly proportional, the constant of proportionality can be determined in the ratio m = F1 / a1, on the other hand if another force of different magnitude say, (F2) is acted on an object, it will create another acceleration say, a2 such that m = F2 / a2… Thus, m serves as the constant of proportionality. Equation of Motion F = ma
  • 7. In the case that 2 or more forces acting on a particle, the resultant force is determined by a vector summation of all the forces. FR = F Generally, the equation of motion is written as F = ma Static Equilibrium: F = 0 FR = F = 0 thus , a = 0 Dynamic Equilibrium: FR = F = ma F – ma = 0
  • 8. Equations of Motion: Rectangular Coordinates In a x,y & z frame of reference, the forces acting on a particle can be expressed in terms of i, j, k components, so we have F = ma Fx i + Fy j + Fz k = m ( ax i + ay j + az k ) To satisfy the given condition with its respective i, j, k components: Fx = max Fy = may Fz = maz
  • 9. F R I CT I O N : If the particle contacts on rough surface, it is necessary to use the frictional equation, which relates the coefficient of Kinetic Friction µk to the magnitude of the Frictional Force (Ff) and Normal Force (N) acting on the surface of contact, Ff = µk N Where: Ff - frictional force acting opposite the subjected Force µk - coefficient of kinetic friction N - normal force - force acting perpendicular to the point of contact.
  • 10. The 50 kg crate rests on a horizontal plane for which the coefficient of kinetic friction is µk = 0.3 . If the crate is subjected to a 400-N towing force 30⁰ from the horizontal, determine the velocity of the crate in 5 sec starting from rest. EXAMPLE # 1
  • 11. The 100 kg block A is released from rest. If the mass of the pulleys and the cord are neglected, determine the speed of the 20 kg block B in 2 seconds. EXAMPLE # 2
  • 12. At a given instant the 10 kg block A is moving downward with a speed of 6 m/s. determine its speed 2 sec later. Block B has a weight of 4 kg, and the coefficient of kinetic friction between it and the horizontal plane is µk = 0.2 . Neglect the mass of the pulleys and cord. EXAMPLE # 3
  • 13. Determine the time needed to pull the cord at B down 4 m starting from rest when a force of 10 kg is applied to the cord. Block A weighs 20 kg. Neglect the mass of the pulleys and cords. EXAMPLE # 4