Spring Projectile problem: center of mass

AI Thread Summary
The discussion centers on a physics problem involving two masses connected by a massless spring, where one mass is given an upward velocity. The user seeks to determine the position of the masses over time, having already calculated the center of mass motion. They recognize the need to analyze the system as an oscillatory motion but struggle to find the amplitude and the positions relative to the center of mass. Another participant emphasizes the importance of considering potential energy in the spring and notes that the equations provided assume no normal force from the ground, complicating the analysis if such a force is present. Understanding these dynamics is crucial for accurately solving the problem.
Zenshin
Messages
5
Reaction score
0
Hello everyone. I'm burning my head at this one, maybe someone could offer some insight? Here's the deal: imagine two masses, m1 and m2, united by a massless spring, of length l (relaxed).

m1
|
| _ > spring, at length l (relaxed)
|
___m2____ ground

The system has this config at rest. Then, it'f given a velocity v , upward, to the mass m1, and the question is: what is the position of the masses in any given time? I've figured out that I've to break the problem in two parts: find out the center of mass motion and then determine the position of the masses relative to it. However, how can I do that? I've already found out the center of mass motion, but I can't find the position of the masses relative to it. I assume it's a oscillatory motion, but I can't find it's amplitude. The only thing I have is the initial velocity of the mass m1, nothing else. Please, any advice would be HIGHLY useful hehehe

Thanks in advance!
 
Physics news on Phys.org
All right:
Let us set up the individual laws of motion here:
-m_{1}g-k(x_{1}(t)-x_{2}(t)-l)=m_{1}a_{1}
-m_{2}g+k(x_{1}(t)-x_{2}(t)-l)=m_{2}a_{2}
where x_{1},x_{2} are the respective positions of the masses, with associated accelerations a_{1},a_{2}
This is a second-order linear system with constant coefficients which is readily solvable.
 
since the motion is vertical, we use y instead of x (y positive upward). We divide this soution into two parts. 0.5mv1^2 + mgy1 = 0.5mv2^2 + mgy2
0 + mgh = 0.5mv2^2 + 0
v2 = squ root2gh)
 
klmdad said:
since the motion is vertical, we use y instead of x (y positive upward). We divide this soution into two parts. 0.5mv1^2 + mgy1 = 0.5mv2^2 + mgy2
0 + mgh = 0.5mv2^2 + 0
v2 = squ root2gh)
Whatever are you talking about?
Where, for example, have you included the potential energy of the system contained in the spring?

Zenshin:
While I believe that the equations given are the ones you were asked to find, nevertheless it is important to realize that these equations are only valid under the assumption NO NORMAL FORCE ACTING ON THE SYSTEM FROM THE GROUND. If you want to include the possibility of a non-zero normal force as well, you've got a much trickier situation.
 
Thread 'Voltmeter readings for this circuit with switches'
TL;DR Summary: I would like to know the voltmeter readings on the two resistors separately in the picture in the following cases , When one of the keys is closed When both of them are opened (Knowing that the battery has negligible internal resistance) My thoughts for the first case , one of them must be 12 volt while the other is 0 The second case we'll I think both voltmeter readings should be 12 volt since they are both parallel to the battery and they involve the key within what the...
Thread 'Correct statement about a reservoir with an outlet pipe'
The answer to this question is statements (ii) and (iv) are correct. (i) This is FALSE because the speed of water in the tap is greater than speed at the water surface (ii) I don't even understand this statement. What does the "seal" part have to do with water flowing out? Won't the water still flow out through the tap until the tank is empty whether the reservoir is sealed or not? (iii) In my opinion, this statement would be correct. Increasing the gravitational potential energy of the...
Back
Top