Everyday I'm jugglin'

A juggler is juggling with four balls. He tosses and catches two at a time so that the interval between the two tosses is maximal and constant, t = 0.4 s t = 0.4~\mbox{s} . Each ball is tossed with the same initial velocity, so that it makes a parabolic path to his other hand. The distance between his hands is d = 50 cm d = 50~\mbox{cm} and they are at a same height. What should be the initial speed of the balls in m/s so that they can reach up to h = 78.4 cm h=78.4~\mbox{cm} in height?

Details and assumptions

  • Assume the juggler tosses the balls right after he catches them.
  • There are no other forces but gravity that act on the balls.
  • Acceleration due to gravity is 9.8 m/s 2 -9.8~\mbox{m/s}^2 .


The answer is 3.97.

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4 solutions

Ahaan Rungta
Sep 15, 2013

Let the initial speed be v v . Let the horizontal component be v x v_x and the vertical component be v y v_y . We know that v 2 = v x 2 + v y 2 , v^2 = v_x^2 + v_y^2, so we need to obtain v x v_x and v y v_y , so that we can calculate v v .

Vertical Motion : We have that v y 2 = 2 g h . v_y^2 = 2gh. This is simply because the y y -velocity at the peak is 0 0 . We will need to find the time of flight for future reference. To do this, note that h = 1 2 g t 2 , h = \dfrac {1}{2}gt^2, where t t is the time to reach the peak of the trajectory. We obtain t = 2 h g . t = \sqrt {\dfrac {2h}{g}}. By symmetry, the time of flight is 2 t = 2 2 h g 2t = 2 \cdot \sqrt {\dfrac {2h}{g}} .

Horizontal Motion : The projectile travels horizontally a distance d = 0.50 m d = 0.50 \, \text{m} in a time 2 t 2t . Thus, the horizontal velocity is v x = d 2 t = d 2 2 h g . v_x = \dfrac {d}{2t} = \dfrac {d}{2 \cdot \sqrt {\dfrac {2h}{g}}}.

Putting it together : v = v x 2 + v y 2 = ( d 2 2 h g ) 2 + 2 g h = g d 2 8 h + 2 g h . \begin{aligned} v &= \sqrt {v_x^2 + v_y^2} \\&= \sqrt {\left( \dfrac {d}{2 \cdot \sqrt {\dfrac {2h}{g}}} \right)^2 + 2gh} \\&= \sqrt {\dfrac {gd^2}{8h} + 2gh}. \end{aligned} Using d = 0.50 m d = 0.50 \, \text{m} , g = 9.8 m/s 2 g = 9.8 \, \text{m/s}^2 , and h = 0.784 m h = 0.784 \, \text{m} , we have v = 3.97 m/s . v = \boxed {\text {3.97 m/s}}.

Alternatively, we could have just numerically calculated v x v_x and v y v_y separately and then used v = v x 2 + v y 2 v = \sqrt {v_x^2 + v_y^2} , but the above also works.

DUDE I FOUND IT JUST BY UT+1/2AT2

Shubham Chaudhary - 7 years, 8 months ago

Just asking i dont get it well, Why v0 is'nt counted? well y-velocity at the peak is 0. but not change the v0 right? and why t=0.4 sec isn't used too?

Hafizh Ahsan Permana - 7 years, 8 months ago

v = v0 + at zero = v0 + [-9.8x.4] v0 = 3.92

Hussein Salah - 7 years, 8 months ago
Jian Feng Gao
Sep 15, 2013

In the y component, we know that vf^2-vi^2=2ad and at the top of the parabola vf=0

We get -vi^2=(2)(-9.8)(0.784)

vi=3.92

in the x component, since the time for 2 tosses is 0.4s, then the amount for 4 tosses, which is the period, must be 0.8s.

vx=0.5/0.8

=0.625

v^2 = vi^2 + vx^2

v^2 =3.92^2 + 0.625^2

Therefore, v=3.97

Shubham Chaudhary
Sep 20, 2013

BY USING THE FOLLOWING EQUATION WE CAN FIND THE INITIAL VELOCITY S=UT+1/2AT2 0.784=0.4U-1/2 9.8 0.4*0.4 0.784=0.4U-0.784 U=1.568/0.4 WE GET U AS 3.97

Since the time between two throws is 0.4, the time of flight is 4*0.4=1.6s. Let θ \theta be the angle at which the ball is thrown. Then, we have the following equations-

u cos ( θ ) t = d u{\cos(\theta)}t=d

1 2 m ( u sin ( θ ) ) 2 = m g h {1 \over 2}m(u\sin(\theta))^2=mgh

Solving, for u u , we get u = 3.9324 u=3.9324 .

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