motion speed acceleration velocity

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    Speed, velocity,

    acceleration & Newton

    Micro-World Macro-WorldLecture 2

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    speed

    speed = v =

    distance traveled

    elapsed time

    50km

    v = 50km

    1 hr  = 50km/hr  

    Hawaii Kai  Haleiwa

    In one hor 

    This is the averagespeed over 1 hour.For shorter timeintervals it can be

    higher or lower.

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    instantaneous speed

    Instantaneous

    speed = here

    ! here

    "peed determined #or ver$ short time intervals

    vistantaneos  =distance traveled!very short" time

    km

    %m %m 

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    Earth’s motion around the Sun

    r=1#5$1011m

    % =distance

    elapsed time  = r $ '#1( $ 1#5 $ 1011m

    ')5 days $ ( hr/day=

    1year 

    =*#( $ 1011 m

    +)0 hr =

    *#( $ 1011 m

    +#) $10' hr 

    = 1#1$10+

    m/hr = 1#1$105

    km/hr  ≈

     11& %m'hr

    *#(

    +#= $ 1011-' m/hr

     =  1  

     -  (  %  m

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    Tip of a watch’s minute hand (HW!!)

    % = distanceelapsed time  = r $ '#1( $ 1cm)0 min $ )0 s/min=1hr 

    =)#+ cm

    ')00 s=

    )#+ cm

    '# ) $10's= 1#$10-' cm/s

    = 1#$10-5 m/s

      r   =   1 

      c  m

    = 1   - 2  

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    Scalars and Vectors

    Simple nm.ers

    Speed v 

    emperatre T 

    Nm.er direction

    %elocity v

    relative positions r 

    2orce 2

    3cceleration a

    4i.rary

    r

      5  a  m

      p    s

      5  e  n   t  e

      r

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    Velocity = speed direction

    r=1#5$1011m

    ) months laterspeed = same

    di##erent direction

    v

    velocit$ is a *vector+, a uantit$ that has bothmagnitude and direction

    Length o# the arrow = speedirection o# arrow same asdirection o# the motion

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     cceleration ( chan"es in #)

    acceleration = change in velocit$elapsed time

    a =

    change in v elapsed time

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    han6e in % = 100km/hr 

    7lapsed time = ' sec

    *This bab$ goes #rom to1%m'hr in onl$ ( seconds+

    a =chan6e in velapsed time

     = 100km/hr ' s  = '' km/hr s10' m

    ')00 s

    ='#)$10's

     =''$10'm

    '#)$10' s$s = *#1 m/s

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    $ifferent ways to chan"e V

    v v

    ar speeds p

    v

    ar slows p

    v

    s c r e e c h ! 

    a

    a

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     ccelerations (continued)

    v

    5 ar  t r nsv   

    In all three cases, v chan6es#here8ore these are all e$amples o8 accelerations

    a

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    a % v on a hot wheels track

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    Free Fall

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    (#*m

    t=0 v0=0

    t=1s v1=9

    vav6 =  disttime

    (#*m1 s=  = (#*m/s

    vav6

     =  v0  v1

    0 v1

    v1

    v1 = vav6 = *#+ m/s

    %1 = *#+ m/s

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    &ree'fall acceleration

    acceleration =chan6e in velocity

    elapsed time

    a =*#+m/s

    1s= *#+ m/s

    /.0m's

    1s

    This is called the *acceleration due to gravit$+ and given the special s$mbol,

    g=/.0m's2

    In this class g≈

    1 m's2

     will be close enough #or us

    g

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    &ree fall from "reater hei"hts

    %0 = 0

    t = 0s

    %1 = 10m/s

    t = 1s

    5m

    % = 0m/s

    t = s

    %' = '0m/s

    t = 's

    %( = (0m/s

    t = (s

    15m

    5m

    '5m

    5m

    0m

    (5m

    +0m

    otal

    distance

    1

    6t

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    pward toss

    %( = 0t = (s

    %' = 10m/st = 's

    5m

    % = 0m/st = s

    %1 = '0m/s

    t = 1s

    %0 = (0m/st = 0

    15m

    5m

    '5m

    5m

    )0m

    '5m

    0m

    otal

    hei6ht

    +0m

    6t1

    v0t

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    "imple rule #or #ree #alla%a, proectile motion

    When Earth’s gravity is the only forceinvolved:

    actual height = height for no gravity 3gt2

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    Hori*ontal tosst = 0s

    t = 1s

    5m

    t = s t = 's t = (s

    0m

    (5m

    +0m

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    upward toss

    t = 0s

    t = 1s

    5m

    t = s

    t = 'st = (s

    0m

    (5m+0m

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    Shoot the monkeycommnistdead white

    4uropean male

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    %ery 8ast hori:ontal toss

    t = 0st = 1s

    $= +km

    5m

    t = s

    $=1)km

    t = 's

    $=(km

    0m (5m

    %=+km/s

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    +r,ital motion is free fall

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    3rti8icial satellite

    a = 6

    v = + km/s

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    Turnin" car 

    5n obect #ree to slide on the dashboard&tries to #ollow a straight line path

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    -ewton’s . laws of motion

    Isaac Newton 1)( --- 1

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    le/ander 0ope1 

    6ature and nature7s laws la$ hid in the night

    8od said& *Let 6ewton be&+ and all was light.

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    2st 3aw1 3aw of 4nertia

    5 bod$ at rest tends to sta$ atrest& a bod$ in motion tends to%eep moving along at a constantspeed and in a straight-line

    path unless inter#ered with b$some e9ternal #orces. 

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    e/ample

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    5otorcycle crash dummy

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     nother e/ample(watch the ladder)

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    2nd Law, F=ma

    T he acceleration o# a bod$ is directl$proportional to the net #orce acting on

    it and inversel$ proportional to itsmass.The direction o# the accelerationis in the direction o# the applied #orce

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    $irectly proportional to &orce

    a

    Small 8orceSmall acceleration

    a

    4ar6e 8orce

    4ar6e acceleration

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    in#ersely proportional to mass

    aa

    4ar6e mass

    Small acceleration

    small mass

    4ar6e acceleration

    ;owlin6

     .all

    ;each

    .all

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    *Inertial+ mass

    *Inertial+ mass& mi& is the resistance tochanges in the state o# motion

    :bects with large mi are hard to get moving;! once started& hard

     to stop

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    nits a"ain! (we cant a#oid them!)

    Mass, basic unit = 1%ilogram = 1%g

      mass o# 1 liter ;1.1 uarts< o# water

    This muchwater

    1cm

    1cm

    1cm

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    -et force

    Tip-to-tail method#or adding vector

    "lide tail o# one to tipo# the other ;%eepdirections #i9ed<

    6et #orce is the vector#rom the tail o# the 1st to

    the tip o# the 2nd. ; inthis case

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    Tip-to-tail method

    "lide tail o# one to tipo# the other ;%eepdirections #i9ed<

    6et #orce pointsdown the hill

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    6ewton7s 2nd law F=ma

    a ∝ F

    a ∝ 1'm

    a is proportional to F,

    direction o# a

    = direction o# F,

    a ∝ F

    a is inversel$proportional to m,

    a ∝ F'mcombine,

    set proportionalit$constant = 1, a = F'm 

    multipl$both sides

     b$

    m

    W i ht & f it

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    Wei"ht = &orce of "ra#ity

    a = 6<

    ;owlin6

     .allm

    ;each

    .all

    a = 621 = ma2 =

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    Wei"ht is proportional to mass

    Newton>s nd law 2=ma

    I8 6ravity is the only 8orce 2 = ?  a = 6

    ? = m6weight

    *gravitational+mass

    accelerationdue to gravit$

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    wo different  aspects o8 mass

    Weight, W = m g Force o# gravit$ isproportional to*gravitational+ mass

    a = F

    m

    Inertia> resistanceto changes in stateis proportional to*inertial+ massmi 

    mgg

    6ewton7s 2nd law,

    49perimentshows, mg = mi 

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    nits of &orce

      F=ma

    %gm

    s2

    ?nit o# #orce, 1 6ewton = 16 = 1 %g m's2

    1 pound =1lb = @.A 6

    What is your mass6

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    What is your mass6

    Weight = #orce o#

    4arth7s gravit$ on $ou

    W=mg

    W

    a=g

    F=ma

    m=Wg

    "uppose I

     ump o##a tble

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    Mass ! weight

    Bonvert to 6ewtons,

    W = 0A %g 9 /.0m's2 = 0(( 6

    %g m's2?nits o# 6 =

    Cg# =*%ilogram #orce+ = /.0 6

      * w

     e i g  h t +

      =  0 A

      % g 

    %g is a unit o# mass& not #orce

      * m $  w

     e i g  h t +

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    6ewton7(rd Law, action-reaction

    Whenever one obect e9erts a #orce on asecond obect& the second obecte9erts an eual in magnitude but

    opposite in direction #orce on the #irst.

    action, I push

    on the canoe

    reaction, thecanoe pushes

    me #orward

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    ActionReaction

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    I push on the bus 

    F

    v=

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    Dut I  accelerate

    6ewton,

    The bus e9erted an *eual but opposite+ #orce on me.

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    Loo% again

    F

    -F

    5ll #orces come in pairs

    This #orce causes meto accelerate bac%wards

    This #orce tries to accel.the bus #orward

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    5ir-#illed balloon

    action, balloonpushes on air

    reaction, airpushes on balloon

    il

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    recoilaction, gun e9erts

    #orce F2 on bulletma%ing it accelerate

    reaction, eual butpposite #orce on the gun F1

    Eroduces a recoil

    7 k t l i

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    7ocket propulsion

    action, roc%et enginepushes e9haust

    gasses out the rear

    reaction, roc%etgets pushed

    in the opposite

    direction