sph3u motion in 2 dimensions river crossing problems...

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RIVER CROSSING PROBLEMS PROJECTILE MOTION SPH3U Motion in 2 Dimensions

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  • RIVER CROSSING PROBLEMS PROJECTILE MOTION

    SPH3U – Motion in 2 Dimensions

  • ADDING VELOCITIES IN 2-DIMENSIONS

    Video – The River Boat Problem The keys to these types of problems:

    Treat the x and y components independently The same time is taken for each motion !!!!!

  • PG. 74 – PRACTICE #2

    BEIKiii'

  • GivenD= 20 . OnFx¥ 2.7 nls [w]Ty = 1 . 3 mls [ N ]

    Required: *dtxAnalysis: Ty . 1}dy= jvxasdx

    t

  • Steps=ddy_ ohiadx

    Itat

    at=y# Edxixat→20 .om[N] ?27÷[Dxk4

    = m|s[N] [d×= 41.58mAst. 15.45 £dxs42m[w]

    bt= loss

  • PROJECTILE MOTION

    Projectile Motion the motion of a projectile under gravity

    Projectile an object that moves along a two-dimensional curved trajectory in response to gravity

    Time of Flight the time taken for a projectile to complete its motion

  • DESCRIBING PROJECTILE MOTION

    2-dimensional vector problems velocity vectors pointing up or to the right have positive values velocity vectors pointing down or to the left have negative values

  • PROJECTILE MOTION – KEY POINTS

    horizontal and vertical motions are independent the horizontal and vertical motions take the same amount of time projectiles move horizontally at a constant velocity projectiles undergo uniform acceleration in the vertical direction ( acceleration due to gravity)

  • PROJECTILE MOTION – KEY POINTS (CON’T)

    objects can be projected horizontally or at an angle to the horizontal projectile motion can begin and end at the same or at different heights use the Big 5 equations of motion to solve projectile motion problems if you know the initial velocity and vertical displacement of the projectile you can solve for time of flight, maximum height, and range.

  • PG. 81 #8

    *→

    t

    Givenszs

    . Tdy = - kmday\Ej9.8÷[dadsur Y

    sdx

    Atiyeh's ,÷ln2D

    Tins 45340525 )

  • -

    RequiredAnalysis sty =D tx

    Edy=hgstttaayat'

    5¥ :.

    hm=4s=¢nz5)attk(98⇒aE

    s

    - Rm : 1.90¥t -4.9mg at'

    0 = - 4.9mg At 't 1.90 ;dtH2m

  • a = -4.9 b= 1.90 c=l2

    Quadratic Formulaat . - b±Tb÷

    Za

    at . t.at#44.HzTtag

    st = -1.90123M¥ao

    at = -1.90+15.4 At= -1.90-15.4a a

    st. -1 .↳s*wAoin$ 's t= ) . >6s✓

  • bty ' - Dtx - . 1.76 sTix = 4 . sz ¢os 25

    ° )tax . Ong OIdx ^

    bdx = riot t §qµt2Idx =(4.sn#cos2sD(h6/DEdx=7.2m

  • WORK FOR THE DAY

    Pg. 78-81 – go over Sample Problem #1 and #2 Any issues with pg. 75 #8 and 9 ??? Pg. 81 #2, 4-7 Unit Test on Friday !! Quiz 6 this Wednesday

    •"