Horizontally launched projectile

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SUMMARY

The discussion focuses on the physics of a bomb launched horizontally from a plane, analyzing its trajectory concerning the ground, the plane, and vice versa. Key equations utilized include the SUVAT equations, specifically ##y(t) = y_0 + v_{0,y} t - \frac{1}{2} g t^2##, where ##y_0## represents the initial height. Participants clarify the relationship between the velocities of the bomb and the plane, leading to the conclusion that the position vector can be expressed as ##\vec r = ut + h - \frac{1}{2}gt^2##. Additionally, Galilean transformations are discussed as a method for solving the problem.

PREREQUISITES
  • Understanding of projectile motion and its equations, specifically SUVAT equations.
  • Familiarity with vector notation and operations in physics.
  • Knowledge of Galilean transformations and their application in classical mechanics.
  • Basic concepts of kinematics, including initial velocity and acceleration due to gravity.
NEXT STEPS
  • Study the application of SUVAT equations in various projectile motion scenarios.
  • Learn about vector addition and subtraction in the context of physics problems.
  • Explore Galilean transformations in more depth, particularly their use in relative motion problems.
  • Practice solving similar problems involving horizontal launches and relative motion between objects.
USEFUL FOR

Students studying physics, particularly those focusing on kinematics and projectile motion, as well as educators seeking to clarify concepts related to relative motion and trajectory analysis.

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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