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    Projectiles (1)Object projected vertically upwards1. Maximum height reached (H) = ½ gt = u!g

    . "t a#y other height except the maximum$h = ut %½gtspace v = u %gh spa where g = & '. ms&

    Object projected horio#tally

    *he horio#tal dista#ce travelled (s) = horio#tal velocity x time = vxt = ut

    *he vertical dista#ce travelled (h) = uyt % ½ (gt) = ½ (gt) si#ce uy = +

    ,elocity a-ter a time t$ space v = (vx % vy

    )1!

    irectio# o- motio# a-ter time t$ space ta#θ = vy!vx/0uatio# -or the path$ spaceh = ½ (gt) = ½ (gs!u) = s( ½ )(g!u)

     

    Projectiles (2)Object projected at an angle A to the horizontal(a) RangeRange (R) = horizontal velocity x time = !cos A x 2! sin A"#g =!22 sin A cos A"#g

    Range (R) = !2sin 2A#g

    $he maxim!m range %or a given velocity o% projection &ill be &hensin 2A = 1' that is' &hen 2A = o or &hen A = *+o

    (b) ,eight$he projectile &ill reach its maxim!m height &hen the vertical

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    component o% its velocity is zero' that is' &hen ! sin A - gt = ' or&hen t = ! sin A#g"

    .axim!m height (,) =

    !2sin2A"#2g