Horizontally launched projectile

AI Thread Summary
The discussion revolves around the analysis of a bomb launched horizontally from a plane, focusing on its trajectory relative to both the ground and the plane. Participants clarify the use of initial height (y₀) and the equations of motion (SUVAT) to derive the bomb's trajectory. They also discuss the relative motion between the bomb and the plane, emphasizing the need to consider vector components. The conversation touches on the application of Galilean transformations to solve the problem. Overall, the participants are collaboratively working through the physics concepts to arrive at the correct trajectory equations.
Davidllerenav
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Homework Statement


A bomb is launched from the front of a plane horizontally. The inicial velocity of the bomb is ##v##, the inicial velocity of the plane is ##u##. Find:
  1. The trayectory of the bomb with respect to the ground.
  2. The trayectory of the bombb with respect to the plane.
  3. The trayectory of the plane with respect to the bomb.

Homework Equations


SUVAT

The Attempt at a Solution


I tried the first one like is shown in the picture. Is it right? How do I solve the others?
 

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Hi,

Nice realistic sketch of the plane :smile:
I miss ##y_0## in your last line ? Where is ##y = 0## ?

re part 2: How about ##\ \vec r_{\rm bomb}- \vec r_{\rm plane} ## ?
 
BvU said:
Hi,

Nice realistic sketch of the plane :smile:
I miss ##y_0## in your last line ? Where is ##y = 0## ?

re part 2: How about ##\ \vec r_{\rm bomb}- \vec r_{\rm plane} ## ?
Thanks. What do you mean by ##y_0##? Isn't it equal to h?. Why ##y=0##?
For the secon one I did ##v_{b/p}=v-u##, you are doing the same but with the positions, right?
 
SUVAT says ##y(t) = y_0 + v_{0,y} t - {1\over 2} g t^2##. Your picture suggests ##y_0 = h##

Davidllerenav said:
For the second one I did
I don't know what you did, only what you asked
Davidllerenav said:
How do I solve the others?
 
upload_2019-2-17_23-34-41.png

could you read aloud the last line for me :rolleyes: ?
 

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BvU said:
SUVAT says ##y(t) = y_0 + v_{0,y} t - {1\over 2} g t^2##. Your picture suggests ##y_0 = h##
Yes, that's why ##y(t)=h-\frac{1}{2}gt^{2}##, since ##v_{0y}=0##
BvU said:
I don't know what you did, only what you asked
I said that the speed of the bomb with respect to the plane is the speed of the bomb- the speed of the plane.
BvU said:
View attachment 238918
could you read aloud the last line for me :rolleyes: ?
It means that the position vector is the sum of the position on the x-axis which is ##x(t)=v_0t=ut## and the position on the y-axis which is ##y(t)=h-\frac{1}{2}gt^{2}##. Thus the trayectory would be given by ##\vec r= ut+h-\frac{1}{2}gt^{2}##.
 
Well well, I had difficulty reading the +h in the last line.

##y(t)=h-\frac{1}{2}gt^{2}## is good. So is ##x(t) = ut##. But I resent $$r = ut +h - g{t^2\over 2}\ .$$You can not add ##ut## and ##h-g{t^2\over 2}## as if they are numbers.
 
BvU said:
Well well, I had difficulty reading the +h in the last line.

##y(t)=h-\frac{1}{2}gt^{2}## is good. So is ##x(t) = ut##. But I resent $$r = ut +h - g{t^2\over 2}\ .$$You can not add ##ut## and ##h-g{t^2\over 2}## as if they are numbers.
I must add the ##\vec i## and ##\vec j## unit vectors right?
 
Yes. And then ##\vec r ## is a vector again.
 
  • #10
BvU said:
Yes. And then ##\vec r ## is a vector again.
Ok. So the first one is done. Now I just need to do ##\ \vec r_{\rm bomb}- \vec r_{\rm plane}## as you said for the second part right?
 
  • #11
I agree. You're doing fine. Bedtime for me :sleep:
 
  • #12
BvU said:
I agree. You're doing fine. Bedtime for me :sleep:
Ok, thanks! One last question, for the third part, I just need to do the same thing from the second part but it would be ##\ \vec r_{\rm plane}- \vec r_{\rm bomb}##, right?
 
  • #13
BvU said:
I agree. You're doing fine. Bedtime for me :sleep:
Can this problem be solved using Galilean transformations?
 
  • #14
Yes :smile:
 
  • #15
BvU said:
Yes :smile:
And how would it be if we solve it with Galilean transformations?
 
  • #16
BvU said:
Yes :smile:
I ended up with ##\vec r = (V-U)t \vec i -(g\frac{t^{2}}{2})\vec j## in the case of the bomb with respect to the plane, and ##\vec r = (U-V)t \vec i +(g\frac{t^{2}}{2})\vec j## in the case of the plane with respect to the bomb, am I right?
 
  • #17
One way to find out: hand it in ! :cool:
 
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