Chapter 3-Acceleration and Newton Second Law of Motion

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    C GH C, . .

    Chapter 3

    UNIT 5Section 3.1

    Section 3.2Section 3.3

    Section 3.4

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    POSITION AND DISPLACEMENT

    2

    Introduction to Newtons Second Law of Motion

    In the previous chapter 2, we concentrated on situations in

    which the net force acting on an object is zero. When anonzero net force acts on an object, the velocity changes.

    Newtons second law of motion (presented in Section 3.3)tells us how the net force and the objects mass determine the

    change in velocity.

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    POSITION AND DISPLACEMENT

    3

    ,

    . , ,

    ( ).

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    POSITION AND DISPLACEMENT

    4

    .

    D .

    .

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    positioninitial=o

    x

    r

    positionfinal=xr

    ntdisplaceme==

    o

    xxx

    rrr

    Displacement is a vector quantity.

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    m0.2=o

    x

    r

    m0.7=xr

    m0.5=xr

    m0.5m2.0m7.0 === oxxxrrr

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    Example 3.2

    7

    C, C

    27 18 ,

    17 G, 13 48

    C.

    ?

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    Example 3.2

    8

    A

    A

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    Example 3.2

    9

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    Example 3.2

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    Example 3.2

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    Speed and Velocity

    Average speed is the distance traveled divided by the timerequired to cover the distance.

    timeElapsed

    DistancespeedAverage =

    SI units for speed: meters per second (m/s)

    and speed is a scalar quantity.

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    Average velocity is the displacement divided by the elapsed

    time.

    timeElapsedntDisplacemevelocityAverage =

    ttt o

    o

    =

    =

    xxx

    v

    rrr

    r

    Speed and Velocity

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    14

    .

    ,

    . H,

    .

    Speed and Velocity

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    The instantaneous velocity indicates how fast

    an object moves and the direction of motion at each

    instant of time.

    tt =

    xv

    r

    r

    0lim

    Velocity

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    16

    Velocity

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    17

    Velocity

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    ExampleAndy Green in the carThrustSSCset a world record of 341.1 m/s in 1997.To establish such a record, the driver makes two runs through the course,one in each direction, to nullify wind effects. From the data, calculate theaverage velocity for each run.

    Velocity

    sm5.339s4.740

    m1609+=

    +=

    =

    t

    x

    v

    r

    r

    sm7.342s4.695m1609 ==

    =t

    xv

    r

    r

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    Example 3.4

    19

    / = 40 .

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    Example 3.4

    20

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    VELOCITY

    21

    .

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    ACCELERATION AND NEWTONS SECOND

    LAW OF MOTION

    22

    ,

    :

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    The notion of acceleration emerges when a change in velocity is

    combined with the time during which the change occurs.

    ACCELERATION

    ttto

    o

    =

    =

    vvv

    a

    rrr

    r

    DEFINITION OF AVERAGE ACCELERATION

    Average Acceleration is the rate at which the velocity changes

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    Example 3 Acceleration and Increasing Velocity

    Determine the average acceleration of the plane.

    sm0=o

    v

    r

    hkm260=vr

    s0=ot s29=t

    s

    hkm0.9

    s0s29

    hkm0hkm260+=

    =

    =

    o

    o

    tt

    vv

    a

    rr

    r

    ACCELERATION

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    ACCELERATION

    Acceleration and increasing velocity

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    Acceleration and Decreasing

    Velocity

    2sm0.5s9s12

    sm28sm13=

    =

    =

    o

    o

    tt

    vv

    a

    rr

    r

    ACCELERATION

    Whenever the acceleration

    and velocity vectors have

    opposite directions, the objectslows down and is said to be

    deccelerating.

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    27

    F

    :

    ACCELERATION

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    28

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    2sm6s2

    sm12Slope +=

    +=

    =

    t

    v

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    Example 3.6

    31

    A 8.94 /; 120.0 15.0

    7.15 /.

    () ?

    () 120.0 ?

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    Example 3.6

    32

    1.79 / (=8.94 /7.15/).

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    Example 3.6

    33

    ()

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    Example 3.6

    34

    ()

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    Example 3.6

    35

    ()

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    36

    (),

    ().

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    37

    (/)/ = /2.

    , ,

    1 1 1 /2 :1 = 1 /2

    NEWTONS SECOND LAW OF MOTION

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    NEWTON S SECOND LAW OF MOTION

    38

    .

    . .

    .

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    39

    D ( ) .

    .

    .

    D FBD .

    C .

    , (

    ) .

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    40

    F .

    .

    .

    3 4 APPLYING NEWTONS LAWS

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    3.4 APPLYING NEWTON S LAWS

    41

    .

    E 3.10,

    .

    ,

    ; , .

    , ,

    .

    3 8

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    3.8

    42

    B , .

    40.0 .

    36.0 B 65.0 .

    3 8

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    3.8

    43

    () ?

    ()

    = 0.13, .

    () B

    65.0 40.0 ?() ,

    0.5 /?

    3 8

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    3.8

    44

    ()

    3 8

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    3.8

    45

    ()

    ()

    0.3 /2 +.

    ()

    3 9

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    3.9

    46

    A 1.0 30.0

    .

    ,

    0.90 ? .

    3 9

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    3.9

    47

    3 9

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    3.9

    48

    4.4 / 30.0 .

    3 10

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    3.10

    49

    A ,

    90.0 . 15.0

    / 5.00 .

    A

    ,

    ?

    .

    3 10

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    3.10

    50

    3 10

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    3.10

    51

    3 10

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    3.10

    52

    3 11

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    3.11

    53

    F. 3.39 , ; .

    1= 26.0 2= 42.0 , ?

    3.11

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    3.11

    54

    3.11

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    3.11

    55

    3.11

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    56

    Additional examples - A

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    Two different boxes of masses M = 125 kg and m = 45 kg are sliding

    down a rough surface inclined = 35, as shown in the figure below. If

    the coefficients of kinetic friction between the big and small boxes and

    the inclined surface are 0.3 and 0.5 respectively, calculate theacceleration of the two boxes and the contact force between them.

    dd t o a e a p es

    Additional examples - B

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    Two objects with mass m1 = 3 kg and m2 = 2 kg are connected by amassless string that runs over an ideal pulley moves on two frictionless

    surfaces, as shown in the figure below. The inclined surface at the left is

    tilted at an angle 1 = 45 with respect to the horizontal, and surface at

    the right at 2 = 60. Calculate the:(i) Magnitude of the acceleration of the two objects, and

    (ii) Magnitude of the tension on the string.

    p