Is the final velocity of a Tossed tomato the same as its initial velocity

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Discussion Overview

The discussion revolves around the final and initial velocities of a tossed tomato, exploring concepts of energy conservation, momentum, and the effects of gravity. Participants examine the mechanics of the tomato's motion, including its kinetic and potential energy, as well as the implications of the Earth's motion in relation to the tomato.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants assert that the kinetic energy of the tomato at the launch point is equal to its kinetic energy upon return, questioning how this is possible.
  • Others reference the conservation of energy, stating that the total energy remains constant throughout the motion of the tomato in a gravitational field.
  • Some participants propose that the tomato's upward motion can be explained by applying Newton's second law, suggesting that a force was applied to accelerate the tomato.
  • There are discussions about whether the Earth moves in relation to the tomato, with some arguing that conservation of momentum implies the Earth does move slightly.
  • One participant suggests that the final velocity of the tomato would only equal its initial velocity if the net momentum transferred to it was zero, which is typically not the case.
  • Another participant emphasizes that while speeds may be similar under ideal conditions, the direction of the velocity vector must be considered.

Areas of Agreement / Disagreement

Participants express a range of views on the relationship between the initial and final velocities of the tomato, with some asserting they are identical under certain conditions, while others highlight the complexities introduced by factors like momentum and external forces. No consensus is reached regarding the implications of these factors.

Contextual Notes

The discussion includes assumptions about ideal conditions, such as neglecting wind resistance and treating the gravitational field as constant. There are also unresolved questions about the implications of momentum conservation on the motion of both the tomato and the Earth.

Who May Find This Useful

This discussion may be of interest to students and enthusiasts of physics, particularly those exploring concepts of motion, energy conservation, and the interactions between objects in a gravitational field.

rudransh verma
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When a tomato is thrown up with a velocity ##v_0## it’s kinetic energy is 1/2mv_0^2. It will stop at the top and then again comes back to the launch point where it’s kinetic energy will be same as before, 1/2mv_0^2. How is this possible?

Also when we throw the tomato up how can you be so sure that it’s the tomato that is rising and not that the Earth is going down away from the tomato ?
 
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That's the energy-conservation law (see the other thread on the work-energy theorem). It says that for the motion of a particle (take the tomato as a "particle" here) in the gravitational field of the Earth (approximated as constant) the total energy
$$E=E_{\text{kin}}+V=\frac{m}{2} \vec{v}^2 + m g z=\text{const}.$$
First of all if the tomato starts at ##(x,y,z)=(0,0,0)## with velocity ##\vec{v}_0=(0,0,v_0)## these initial conditions tell you that
$$E=\frac{m}{2} v_0^2 = \frac{m}{2} v^2 + m g z=\text{const}.$$
This tells you that the maximum value ##z_{\text{max}}=h## is reached when ##v=0##, i.e., for
$$\frac{m}{2} v_0^2 = m g h \; \Rightarrow \; h=\frac{v_0^2}{2 g}.$$
At this point the particle must fall down again. If it again reaches ##z=0##, it's velocity must again be ##v_0##.

Note that all this you can read off the energy-conservation law without solving the equations of motion.
 
If we ignore wind resistance, yes..
rudransh verma said:
When a tomato is thrown up with a velocity ##v_0## it’s kinetic energy is 1/2mv_0^2. It will stop at the top and then again comes back to the launch point where it’s kinetic energy will be same as before, 1/2mv_0^2. How is this possible?
Because the math says so? Because parabolas are clearly symmetrical? Because God was too lazy to make it more complicated?

I don't know what sort of answer will satisfy a question like "how is this possible?" when you have the math right in front of you.
Also when we throw the tomato up how can you be so sure that it’s the tomato that is rising and not that the Earth is going down away from the tomato ?
That can get complicated but the easy answer is that the tomato had a force applied so by f=ma we know it accelerated. If you want you can apply that to Earth and see if it makes a difference to ignore it.
 
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vanhees71 said:
That's the energy-conservation law (see the other thread on the work-energy theorem). It says that for the motion of a particle (take the tomato as a "particle" here) in the gravitational field of the Earth (approximated as constant) the total energy
$$E=E_{\text{kin}}+V=\frac{m}{2} \vec{v}^2 + m g z=\text{const}.$$
First of all if the tomato starts at ##(x,y,z)=(0,0,0)## with velocity ##\vec{v}_0=(0,0,v_0)## these initial conditions tell you that
$$E=\frac{m}{2} v_0^2 = \frac{m}{2} v^2 + m g z=\text{const}.$$
This tells you that the maximum value ##z_{\text{max}}=h## is reached when ##v=0##, i.e., for
$$\frac{m}{2} v_0^2 = m g h \; \Rightarrow \; h=\frac{v_0^2}{2 g}.$$
At this point the particle must fall down again. If it again reaches ##z=0##, it's velocity must again be ##v_0##.

Note that all this you can read off the energy-conservation law without solving the equations of motion.
So your second eqn says a lot of things like the initial kinetic energy changes to sum of potential and kinetic energies at some other instant and this sum is always constant. For max h we need v=0. At this point all of the initial kinetic energy changes to potential energy. With this energy it comes down and at z=0 v=v_0.
 
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russ_watters said:
If you want you can apply that to Earth and see if it makes a difference to ignore it.
@rudransh verma : This is worth doing at least one or two times. Especially for a student who doesn't like to take things for granted just because someone says so. You will need to know, the Earth's mass is 6*10^24 kg, and you can pick a mass for the tomato (0.125 kg maybe?).
 
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gmax137 said:
@rudransh verma : This is worth doing at least one or two times. Especially for a student who doesn't like to take things for granted just because someone says so.
For the second trial I suggest the Moon instead of a tomato.
 
rudransh verma said:
I have a better idea. See my post
Thread 'To displace Earth from its orbit'
OK, but I don't see where you have worked out the answer to your question there. The point of my suggestion is that YOU work it out, that's how each of us has learned physics.
 
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rudransh verma said:
How is this possible?
Conservation of energy as explained by @vanhees71 . Don't forget that you have gravity (a force) that acts constantly on the tomato, hence the deceleration on the way up followed by an acceleration in the opposite direction.
rudransh verma said:
Also when we throw the tomato up how can you be so sure that it’s the tomato that is rising and not that the Earth is going down away from the tomato ?
Conservation of momentum together with conservation of energy. In the following problem, replace one cart with your tomato and the other one with the Earth and find out the velocity of each one:

 
  • #10
rudransh verma said:

Is the final velocity of a Tossed tomato the same as its initial velocity​

Commenting on the title instead of the posts:

The final velocity would be the same as the initial velocity only if the net momentum transferred to the tomato over the duration of the flight was zero. This is usually not the case with a tossed tomato, so while the speed might be similar if there had been no wind resistance (conservation of energy and all) and net altitude change, the velocity would tend more towards downward instead of its initial upward trajectory.

rudransh verma said:
Also when we throw the tomato up how can you be so sure that it’s the tomato that is rising and not that the Earth is going down away from the tomato ?
Actually, the Earth does go down and back up a bit. Conservation of momentum demands it.
 
Last edited:
  • #11
Actually the speeds would be identical, with all the caveats from the above posts. Velocity is a vector quantity.
 

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