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PROGRAM OF “PHYSICS” PROGRAM OF “PHYSICS” Lecturer : Dr. DO Xuan Hoi Room 413 E-mail : [email protected]

PROGRAM OF “PHYSICS”

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 PROGRAM OF “PHYSICS”. Lecturer : Dr. DO Xuan Hoi Room 413 E-mail : [email protected]. PHYSICS I (General Mechanics). 02 credits (30 periods) Chapter 1 Bases of Kinematics  Motion in One Dimension  Motion in Two Dimensions Chapter 2 The Laws of Motion - PowerPoint PPT Presentation

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Page 1: PROGRAM OF “PHYSICS”

PROGRAM OF PROGRAM OF “PHYSICS”“PHYSICS”Lecturer: Dr. DO Xuan Hoi

Room 413E-mail : [email protected]

Page 2: PROGRAM OF “PHYSICS”

PHYSICS I PHYSICS I (General Mechanics) (General Mechanics)

02 credits (30 periods)02 credits (30 periods)

Chapter 1 Bases of KinematicsChapter 1 Bases of Kinematics

Motion in One Dimension Motion in One Dimension

Motion in Two DimensionsMotion in Two Dimensions

Chapter 2 The Laws of Motion Chapter 2 The Laws of Motion

Chapter 3 Work and Mechanical EnergyChapter 3 Work and Mechanical Energy

Chapter 4 Linear Momentum and CollisionsChapter 4 Linear Momentum and Collisions

Chapter 5 Rotation of a Rigid Object Chapter 5 Rotation of a Rigid Object About a Fixed Axis About a Fixed Axis

Chapter 6 Static EquilibriumChapter 6 Static Equilibrium

Chapter 7 Universal GravitationChapter 7 Universal Gravitation

Page 3: PROGRAM OF “PHYSICS”

References :References :

Halliday D., Resnick R. and Walker, J. Halliday D., Resnick R. and Walker, J. (2005), Fundamentals of Physics, (2005), Fundamentals of Physics, Extended seventh edition. John Willey Extended seventh edition. John Willey and Sons, Inc.and Sons, Inc.

Alonso M. and Finn E.J. (1992). Physics, Alonso M. and Finn E.J. (1992). Physics, Addison-Wesley Publishing CompanyAddison-Wesley Publishing Company

Hecht, E. (2000). Physics. Calculus, Second Hecht, E. (2000). Physics. Calculus, Second Edition. Brooks/Cole.Edition. Brooks/Cole.

Faughn/Serway (2006), Serway’s College Faughn/Serway (2006), Serway’s College Physics, Brooks/Cole.Physics, Brooks/Cole.

Roger Muncaster (1994), A-Level Physics, Roger Muncaster (1994), A-Level Physics, Stanley Thornes.Stanley Thornes.

Page 4: PROGRAM OF “PHYSICS”

http://ocw.mit.edu/OcwWeb/Physics/index.htmhttp://www.opensourcephysics.org/index.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/HFrame.htmlhttp://www.practicalphysics.org/go/Default.htmlhttp://www.msm.cam.ac.uk/http://www.iop.org/index.html...

Page 5: PROGRAM OF “PHYSICS”

PHYSICS IPHYSICS IChapter 4Chapter 4

Linear Momentum and CollisionsLinear Momentum and Collisions

Linear Momentum and Its Conservation

Collisions in One Dimension

Two-Dimensional Collisions

The Center of Mass

Motion of a System of Particles

Page 6: PROGRAM OF “PHYSICS”

1 1 Linear Momentum and Its Conservation From Newton’s laws: force must be present to From Newton’s laws: force must be present to

change an object’s velocity (speed and/or direction)change an object’s velocity (speed and/or direction)Wish to consider effects of collisions and Wish to consider effects of collisions and

corresponding change in velocitycorresponding change in velocity

Method to describe is to use concept of Method to describe is to use concept of linear linear momentummomentum

scalar vector

Linear momentum = product of mass velocityLinear momentum = product of mass velocity

Golf ball initially at rest, so some of the KE of club transferred to provide motion of golf ball and its change in velocity

p mv????????????????????????????

kg.m/kg.m/ss

Page 7: PROGRAM OF “PHYSICS”

Linear momentumLinear momentum : Vector quantity : Vector quantity, the , the direction of the momentum is the same as the direction of the momentum is the same as the

velocity’svelocity’s

Applies to three-dimensional motion as wellApplies to three-dimensional motion as well; ;x x y y z zp mv p mv p mv

Force and linear Force and linear momentummomentum ( )dv d mv

F ma mdt dt

????????????????????????????

dp Fdt??????????????

Impulse :Impulse :f

i

t

t

I p dp F t ??????????????

dpF

dt

??????????????

Page 8: PROGRAM OF “PHYSICS”

TestTest

Suppose a ping-pong ball and a bowling ball are rolling toward you. Both have the same momentum, and you exert the same force to stop each. How do the time intervals to stop them compare?

1. It takes less time to stop the ping-pong ball.2. Both take the same time.3. It takes more time to stop the ping-pong ball.

Page 9: PROGRAM OF “PHYSICS”

EXAMPLE 1EXAMPLE 1

(a)

A 50-g golf ball at rest is hit by “Big Bertha” club with

500-g mass. After the collision, golf leaves with velocity of

50 m/s. (a) Find impulse imparted to ball(b) Assuming club in contact with ball for 0.5 ms,

find average force acting on golf ball

(b)

0.050 50 0 2.50kg m s kg m s fip mv mv

pF

t

33

2.505.00 10

0.5 10kg m s

Ns

Page 10: PROGRAM OF “PHYSICS”

Conservation of momentum for a two-particle system

1 221 12

( ) ( );

d p d pF F

dt dt

Newton’s third law :

Consider two particles 1 and 2 interacting with each other :

21 12 ;F F

1 2( ) ( )d p d pdt dt

1 2( )0 ;

d p pdt

1 2p p const

In general, for an isolated system :

ii

p const

Whenever two or more particles in an isolated system

interact, the total momentum of the system remains constant

Page 11: PROGRAM OF “PHYSICS”

EXAMPLE 2EXAMPLE 2

The initial momentum of the system:

The final momenta of the two pieces:

One-dimensional explosion: A box with mass m = 6.0 kg slides with speed v = 4.0 m/s across africtionless floor in the positive direction of an x axis.The box explodes into two pieces. One piece, with mass m1 = 2.0 kg, moves in the positive direction of the x axisat v1 = 8.0 m/s.What is the velocity of the second piece?

1 1 2 2fp mv mv ip mv

1 1 2 2mv mv mv ;i fp p

2

(6.0 )(4.0 / ) (2.0 )(8.0 / )2.0 /

4.0kg m s kg m s

v m skg

Page 12: PROGRAM OF “PHYSICS”

2 2 Collisions in One Dimension

a. a. Collisions

A cA collisions is a event of two particles’ coming together for

a short time and thereby producing impulsive forces on

each other

The total momentum of an isolated system just before a

collision equals the total momentum of the system just after

the collision

Page 13: PROGRAM OF “PHYSICS”

PROBLEM 1

A car of mass 1800 kg stopped at a traffic light is struck fromthe rear by a 900-kg car, and the two become entangled. Ifthe smaller car was moving at 20.0 m/s before the collision,what is the velocity of the entangled cars after the collision?

SOLUTION

Page 14: PROGRAM OF “PHYSICS”

b. Types of Collisionsb. Types of Collisions

Momentum is conserved in any collisionMomentum is conserved in any collision

What about kinetic energy?What about kinetic energy?

InelasticInelastic collisions collisionsKinetic energy is Kinetic energy is notnot conserved : conserved :

Some of the kinetic energy is converted into other Some of the kinetic energy is converted into other types of energy such as heat, sound, work to types of energy such as heat, sound, work to permanently deform an objectpermanently deform an object

Perfectly inelasticPerfectly inelastic collisions occur when the collisions occur when the objects objects stick togetherstick together

Not all of the KE is necessarily lostNot all of the KE is necessarily lost

lost energyi fKE KE

Page 15: PROGRAM OF “PHYSICS”

Perfectly Inelastic Collisions:Perfectly Inelastic Collisions:

► When two objects stick together after When two objects stick together after the collision, they have undergone a the collision, they have undergone a perfectly inelastic collisionperfectly inelastic collision

► Suppose, for example, vSuppose, for example, v2i 2i = 0. = 0. Conservation of momentum becomesConservation of momentum becomes

1 1 2 2 1 2( )i i fmv mv m m v

1 2

4

3

E.g., if 1000 , 1500 :

(1000 )(50 ) 0 (2500 ) ,

5 1020 .

2.5 10

f

f

m kg m kg

kg m s kg v

kg m sv m s

kg

1 1 1 20 ( )i fmv m m v

Page 16: PROGRAM OF “PHYSICS”

Perfectly Inelastic Collisions:Perfectly Inelastic Collisions:

► What amount of KE lost What amount of KE lost during collision?during collision?

2 21 1 2 2

2 6

1 12 21

(1000 )(50 ) 1.25 102

before i iKE mv mv

kg m s J

21 2

2 6

1( )

21

(2500 )(20 ) 0.50 102

after fKE m m v

kg m s J

60.75 10lostKE J

lost in heat/”gluing”/sound/…

Page 17: PROGRAM OF “PHYSICS”

ElasticElastic collisions collisions

both momentum and kinetic energy are both momentum and kinetic energy are conservedconserved

Typically have two unknownsTypically have two unknowns

Solve the equations simultaneouslySolve the equations simultaneously

1 1 2 2 1 1 2 2

2 2 2 21 1 2 2 1 1 2 2

1 1 1 12 2 2 2

i i ff

i i ff

mv mv mv mv

mv mv mv mv

Page 18: PROGRAM OF “PHYSICS”

EXAMPLE 2EXAMPLE 2A block of mass m1 = 1.60 kg initially moving to the right

witha speed of 4.00 m/s on a frictionless horizontal track

collideswith a spring attached to a second block of mass m2 =

2.10 kginitially moving to the left with a speed of 2.50 m/s. The

springconstant is 600 N/m.(a) At the instant block 1 is moving to the right with a

speed of3.00 m/s, determine the velocity of block 2.

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EXAMPLE 2EXAMPLE 2A block of mass m1 = 1.60 kg initially moving to the right

witha speed of 4.00 m/s on a frictionless horizontal track

collideswith a spring attached to a second block of mass m2 =

2.10 kginitially moving to the left with a speed of 2.50 m/s. The

springconstant is 600 N/m.(b) Determine the distance the spring is compressed at

thatinstant.Conservation of mechanical

energy :

Page 20: PROGRAM OF “PHYSICS”

2 2 Two-Dimensional Collisions

Momentum is conserved in any collision :Momentum is conserved in any collision :

1 1 2 2 1 1 2 2i i ffmv mv mv mv

Page 21: PROGRAM OF “PHYSICS”

Problem Solving StrategyProblem Solving Strategy

Set up coordinate axes and define your velocities with Set up coordinate axes and define your velocities with respect to these axesrespect to these axes

It is convenient to choose the x axis to coincide with It is convenient to choose the x axis to coincide with one of the initial velocitiesone of the initial velocities

Draw and label all the velocities and include all the given Draw and label all the velocities and include all the given informationinformation

Write expressions for the total momentum before and after Write expressions for the total momentum before and after the collision in the x-directionthe collision in the x-direction

Repeat for the y-directionRepeat for the y-directionSolve for the unknown quantitiesSolve for the unknown quantities

If the collision is inelastic, additional information is If the collision is inelastic, additional information is probably requiredprobably required

If the collision is perfectly inelastic, the final velocities If the collision is perfectly inelastic, the final velocities of the two objects is the sameof the two objects is the same

If the collision is elastic, use the KE equations to help If the collision is elastic, use the KE equations to help solve for the unknownssolve for the unknowns

Page 22: PROGRAM OF “PHYSICS”

PROBLEM 2

A 1 500-kg car traveling east with a speed of 25.0 m/s collidesat an intersection with a 2 500-kg van traveling north at a speed of20.0 m/s.Find the direction and magnitude of the velocity of the wreckage after the collision, assuming that the vehicles stick together after the collision.

SOLUTIONStick together : perfectly inelastic collision

Page 23: PROGRAM OF “PHYSICS”

PROBLEM 2

A 1 500-kg car traveling east with a speed of 25.0 m/s collidesat an intersection with a 2 500-kg van traveling north at a speed of20.0 m/s.Find the direction and magnitude of the velocity of the wreckage after the collision, assuming that the vehicles stick together after the collision.

SOLUTION

Page 24: PROGRAM OF “PHYSICS”

PROBLEM 3

In a game of billiards, a player wishes to sink a target ball 2 in the corner pocket as shown in the figure. If the angle to the corner pocket is 35°, at what angle is the cue ball 1 deflected?Assume that friction and rotational motion are unimportant and that the collision is elastic

SOLUTION

Conservation of energy :

1 2m m

Conservation of momentum :

(3)

(1)

(1) and (3) :

Page 25: PROGRAM OF “PHYSICS”

PROBLEM 4

The figure shows two battling robots sliding on a frictionless surface. Robot A, with mass 20 kg, initially moves at 2.0 m/s parallel to the x-axis. It collides with robot B, which has mass 12 kg and is initially at rest. After the collision, robot A is moving at 1.0 m/s in a direction that makes an angle a = 30° with its initial direction. What is the final velocity of robot B?

Page 26: PROGRAM OF “PHYSICS”

SOLUTION

Page 27: PROGRAM OF “PHYSICS”

3. 3. The center of mass

The coordinates of the center of mass of n particles

x1

y1

x2

y2

Page 28: PROGRAM OF “PHYSICS”

The position vector of the center of mass :

The coordinates of the center of mass of n particles

x1

y1

x2

y2

CM

Page 29: PROGRAM OF “PHYSICS”

EXAMPLE 3EXAMPLE 3A system consists of three particles located as

shown inthe figure. Find the center of mass of the system.

Page 30: PROGRAM OF “PHYSICS”

The center of mass of a symmetric system

CM CMCM

CM?

The center of mass of any symmetric object lies on an axis of symmetry and on any plane of symmetry.

Page 31: PROGRAM OF “PHYSICS”

The center of mass of a rigid body

The vector position of the center of mass :

Page 32: PROGRAM OF “PHYSICS”

An object of mass M is in the shape of a right triangle whose

dimensions are shown in the figure. Locate the coordinates of the

center of mass, assuming the object has a uniform mass per unit

area.

EXAMPLE 4EXAMPLE 4

Page 33: PROGRAM OF “PHYSICS”

PROBLEM 5

The figure shows a simple model of the structure of a water mole- cule. The separation between atoms is d = 9.57 10-11 m. Each hydrogen atom has mass 1.0 u, and the oxygen atom has mass 16.0 u. Find the position of the center of mass.

SOLUTION

Page 34: PROGRAM OF “PHYSICS”

PROBLEM 6

A uniform piece of sheet steel is shaped as shown in the figure. Compute the x and y coordinates of the center of mass of the piece

SOLUTION

Page 35: PROGRAM OF “PHYSICS”

4 Motion of a System of Particles4 Motion of a System of ParticlesThe velocity of the center of mass of the system :

The acceleration of the center of mass of the system :

The center of mass of a system of particles of combined mass M moves like an equivalent particle of mass M would move under the influence of the resultant external force on the system