A tennis ball is struck and departs from the racket of Prof. Jacome horizontally with a speed of 30m/s. The ball hits the court at a horizontal distance of 20 m from the racket. How far above the court is the tennis ball when it leaves the racket?
The tennis ball is travelling horizontally with a speed of 30m/s, and ends up 20m away from the racket. This is all we are given.
So, we will assume the racket is \(y_0\) from the ground.
\(y_0{~}-{\rm the~initial~hieght~of~the~ball}\). \(v_{x0}=v_x=30~{\rm m/s}\) (\(v_{x0}=v_x\) because air resistance is neglected) \( x=20\) (distance before landing)
Can you work out the time it takes the ball to travel 20m horizontally?
(You velocity in the horizontal is unchanged, because we neglect air resistance)
For time, can we use t= v - vo / a
No, you don't need any kinematics for this.
Your velocity in the horizontal is 30m/s (and it doesn't change). The distance in the horizontal that you traveled is 20m. So the time is?
(Yes, it is that simple, because the motion in the horizontal and the motion in the vertical are independent of each other.)
\(\displaystyle \frac{\Delta x}{\Delta t}=v_x\) Right? So, \(\displaystyle \Delta t=\frac{\Delta x}{v_x}=\frac{20{\rm m}}{30{\rm m/s}}=?\)
.666 seconds
yes, 2/3 seconds.
(I will use a fraction. I like to use exact values, and as I find the answer, then approximate .... well, in any case, we want the concept, so if you have any conceptual questions, let me know.)
\(\color{black}{\displaystyle v_{y}(t)=v_{y_0}-gt }\) familiar with this?
hmm is what is vy and vy0 in your formula?
Alternatively, \(\color{black}{\displaystyle v=v_{0}-gt }\), and this is for the velocity in the y direction, where g is gravity.
I am using a subscript of y to denote that it is a motion or velocity in the vertical.
In other words, you agree that we can model the velocity in the\(y\) at any time \(t\) with \(\color{black}{\displaystyle v(t)=v_{0}-gt }\)
and the consequence of this equation (via integration) is \(\color{black}{\displaystyle y(t)=(v_{0})t-\frac{1}{2}gt^2+y_0 }\)
This equation models the vertical displacement. Seen this one before?
hmm well if your talking about integration i am not familiar with it. we're still just learning basic physics
No, the equation, \(\color{black}{\displaystyle y(t)=(v_{0})t-\frac{1}{2}gt^2+y_0 }\)
Did you see this (above) equation?
Is this the first time you see this equation, or is it familiar to you?
i dont think ive seen this equation
Oh, it's one of the kinematics, and this is the appropriate equation to use in this case.
Why? Because you are given the time it takes to fall, t=2/3 seconds, you are given y(t)=0 at this time (b/c at this time ball hits the ground). Also you know gravity is 9.8m/s^2, and you know that the initial velocity in the vertical (the \(v_0\)) is 0.
Is this formula the same as y= V0yt+ 1/2 ayt ?
yes, it is the same formula. \(\color{black}{\displaystyle y=v_{0y}+\frac{1}{2}a_yt}\)
Do you know all of the information to plug in, or should we work on this together?
(You are certainly welcome to try it, and I will check you .... wanna do this?)
Yes! i would like to do so
Sure:) Go ahead, and take your time.
How would i go about finding Voy?
First, I want to adjust your formula.
\(\color{black}{\displaystyle y(t)=v_{0y}+\frac{1}{2}a_yt+y_0}\)
This is more appropriate, because the initial displacement in the y, is not 0. And y(t), because this is the height at time t.
As far as the velocity goes, you are given \(v_{0x}\), and \(v_{0y}\) is not mentioned, so we are assuming that initial the ball's speed is perfectly horizontal.
(In other words, your initial velocity in the y, just the instant the ball leave the racket, is equal to 0.)
and knowing this you can just cross \(\color{black}{\displaystyle y(t)=\color{red}{\bcancel{\cancel{\color{black}{v_{0y}}}}}+\frac{1}{2}a_yt+y_0}\)
So, with a zero initial velocity in the y you will have \(\color{black}{\displaystyle y(t)=\frac{1}{2}a_yt+y_0}\)
The time it takes to fall is \(t=2/3{~}{\rm s}\), and at this time you know that \(y(t)=0\) (because this is when the ball reaches the ground). We also know \(\color{black}{\displaystyle a_y=g=-9.8~{\rm m/s^2}}\).
So, there you have it all to find the initial displacement in the vertical, \(y_0\). (This \(y_0\) is the initial height of the ball, and this is the same height at the very instant the ball leaves the racket.)
oh so the Yo would be 20m ?
Please read the question, and tell me what this value (20 m) corresponds to.
You are given everything (I listed) ... all that remains for you is to plug in the information into \(\color{black}{\displaystyle y(t)=\frac{1}{2}a_yt+y_0 }\) and solve for \(y_0\).
Im not sure if i follow you
Its very confusing
Do you understand why it is \(\color{black}{\displaystyle y(t)=\frac{1}{2}a_yt+y_0 }\), (without adding \(v_{0y}t\) to this)?
(Because originally, the equation is \(\color{black}{\displaystyle y(t)=v_{0y}t+\frac{1}{2}a_yt+y_0 }\), however we got rid of that term by noticing something. -- What did we notice?)
Voy is not mentioned in the problem
We noticed that \(\color{black}{\displaystyle v_{0t}=0 }\), because the only velocity that is there, is the velocity in the horizontal (and not in vertical).
And since \(v_{0y}=0\) we can just write the same without \(v_{0y}t\).
For this reason, instead of the original equation, I have now this: \(\color{black}{\displaystyle y(t)=\frac{1}{2}a_yt+y_0 }\)
Can you tell me, what is \(\color{black}{\displaystyle a_y }\) ?
Oooh! ok ok Ay would be the acceleration
Yes, and in this case the acceleration in the vertical is the what?
BTW, COrrection t is squared. \(\color{black}{\displaystyle y(t)=\frac{1}{2}a_yt^2+y_0 }\)
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