00:03
This problem is we have mobility with a high edge, with high edge.
00:13
And we have two balls.
00:15
The first ball will be thrown straight up and get to maximum position and get down.
00:27
This is the first one.
00:29
We have initial velocity here.
00:34
And the second one is after one later from the second later from the first one.
00:40
First one and then we'll free drop from this building and go down to the ground.
00:50
This is the second one.
00:54
This is the first one.
00:57
Then the problem of part a is to want us to find out if the two balls hit the ground at the same time and the height is 20 meters and the what is the velocity of the first one, of the initial velocity of the first ball.
01:24
Okay, this is the problem of part a.
01:32
From this solution, we should understand the equation, the displacement of y will be equal to v0 t minus half g t square.
01:50
Okay, okay, if we set, if we set the ball two need a time, to hit the ground and then the ball one okay would be need the t plus one because the ball two is one second letter from the ball one.
02:32
Then as we know, there are displacements for these two cases, their displacements are the same.
02:42
So that means the delta 4 -1 is equal to delta 2, delta -by -2.
02:53
Therefore, we can say that the 4 -1, there is the initial velocity for the 4 -1 -v -0 and the t plus 1 minus 5g, t plus 1 -2, is equal to 4 -2, the displacement of ball 2.
03:15
Then this will be half g t squared.
03:25
So from here we can get the v0 could be the denominator to the t plus 1, and the numerator could be half g t plus 1 square minus half g t squared so after the arrangement, this equation could be the 5g t plus 1 and 2t plus 1.
04:13
We said the equation to be 1.
04:17
Now, this is the equation to get the initial velocity, but we must know what is t.
04:31
T is the time.
04:34
Okay, is t is time for bought 2.
04:38
Now, how can we find the t? first of all, we understand that for the b2, the vf square could be the 2gh.
04:52
Okay.
04:53
So we know the vf could be the square root 2gh.
05:00
Then we also know that we also know this vf could be the because v0, okay, could be v0, in this condition is 0, so it would be gt.
05:18
Then we know the t could be square root, g2h.
05:30
Now we know the edge for this condition is 20 meters.
05:37
So then we can plug in the number 2 plus 20 and this could be 2 .20 seconds for the t then plug in then substitute this one to equation 1 then we can get the v0 to be 5 9 .8 and the 2 .02 plus 1 2 times 2 .2 then we can get the initial velocity for 1.
06:32
This is a .2 meter per second.
06:41
This is the answer for part a.
06:48
And we can also draw a picture as this one.
06:57
This is position y, and this is t.
07:01
And then the initial the ball one if this is 20 and we can go up and go down and this is the maximum position and this is my maximum position could be 0 .13 second oh no 0 .8 3 second and the 1 second could be here okay and what's the ball 2 if the ball 2 for the first second, it still stays at the 20 meters.
07:47
Then after that, then we will go down to here.
08:00
Okay, this is the graph for the two balls.
08:08
So there is a hint from here.
08:12
If we want to get the two ball to hit the ground at the same time, the first ball at the time equal to 1, the ball must pass over the maximum position of y.
08:33
Then this has the possibility to get the same type to hit the ground for the two balls.
08:43
We will discuss this later.
08:48
Okay, now let's find out the part b.
08:56
What's the part b? the part b is if the we know the initial kind of for the port -a, port 1, and what's the height of the building to get the two ball hit the ground at the same time? okay, for the first case, v0 equal to 0 .206 m per second, and what's the height for this one? okay, now let's calculate this.
09:51
From this equation, a, we can rearrange this equation.
09:57
Could be from one, we can get this equation, v0t plus v0.
10:12
This denominator multiplied for the vlin, v0, and then we can get this one, 2g, 2t, plus 1.
10:30
Then we can get this.
10:38
Then from this one, we can get the t equal to from here, we can get the t could be v0 minus g is equal to half g minus v0.
11:12
And finally, it could be t equal to v0 minus g, half g minus v0.
11:35
This is our equation 3, and this could be our equation 2.
11:56
Okay, here.
12:01
Now, let's find out the t.
12:08
Okay.
12:09
For this one, the case one, the t, plug in the long numbers, v0 right now is 6 .0, 6 minus 0 .9 .8...