Conservation of momentum and SHM of a spring

In summary, a spring with a force constant of 400 N/m is suspended with a 0.200-kg pan attached to its lower end. A 2.2-kg steak is dropped onto the pan from a height of 0.40 m, causing a totally inelastic collision and setting the system into vertical motion. The speed of the pan and steak immediately after the collision can be determined by applying conservation of momentum, as there is no net external force on the system at the instant of collision.
  • #1
boredaxel
19
0

Homework Statement



A spring of negligible mass
and force constant k = 400 N/m is hung vertically, and a 0.200-kg
pan is suspended from its lower end. A butcher drops a 2.2-kg
steak onto the pan from a height of 0.40 m. The steak makes a
totally inelastic collision with the pan and sets the system into ver-
tical SlIM. What are (a) the speed of the pan and steak immedi-
ately after the collision;

Homework Equations



P = Mv


The Attempt at a Solution



I can't really see how linear momentum can be conserved in this case. Doesnt the weight of the steak constitue a net external force on the system? How then can momentum be conserved? I can do the rest of the problem if i clarify this doubt. Thanks
 
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  • #2
At the *instant* the steak collides with the pan, there is no net external force on the pan-steak system. Therefore, one may apply conservation of momentum at the *instant* of the collision to determine the initial velocity of the system. However, as you correctly point out, both immediately before and after the collision there is a net external force acting on the pan-steak system and therefore momentum is not conserved.

Does that make sense?
 
  • #3
But doesn't the weight of the steak constitue a net external force even at the instant of collision?
 
  • #4
boredaxel said:
But doesn't the weight of the steak constitue a net external force even at the instant of collision?
Yes, but it is finite. The collision occurs over a very short period of time [itex]\Delta t[/itex]. If this is sufficiently short, the collision forces [itex]\Delta \boldsymbol{p}/\Delta t[/itex] will be much, much greater in magnitude finite external forces. In the limit of an instantaneous collision, you can ignore those external forces during the collision process because the internal collision forces become infinitely large (they are impulses). The meat+pan system is effectively a closed system during the infinitesimally short collision process. While conservation of kinetic energy does not apply here (the collision is inelastic), conservation of momentum does.
 
  • #5
Thanks for the clarification. I get it now.
 

Related to Conservation of momentum and SHM of a spring

What is conservation of momentum?

Conservation of momentum is a fundamental law of physics that states that the total momentum of a closed system remains constant. This means that the total momentum before an event must equal the total momentum after the event, assuming no external forces are acting on the system.

How does conservation of momentum apply to SHM of a spring?

In SHM (simple harmonic motion) of a spring, the spring oscillates back and forth with a certain momentum. According to the law of conservation of momentum, the total momentum of the spring and any attached objects must remain constant throughout the motion. This means that as the spring compresses and expands, the momentum of the system must also change in order to maintain the overall constant momentum.

What is SHM (simple harmonic motion) of a spring?

SHM is a type of periodic motion in which a system oscillates back and forth around a stable equilibrium position. In the case of a spring, SHM occurs when the spring is stretched or compressed and then released, causing it to vibrate back and forth at a constant frequency.

What factors affect the period of SHM of a spring?

The period of SHM of a spring is affected by the mass of the object attached to the spring, the stiffness of the spring (its spring constant), and the amplitude of the oscillation. A heavier mass, a stiffer spring, and a larger amplitude will result in a longer period.

How is the equation for SHM of a spring derived?

The equation for SHM of a spring, x = A sin(ωt + φ), can be derived using Newton's Second Law of motion and Hooke's Law for a spring. By setting up equations for the forces acting on the mass attached to the spring and solving for acceleration, we can arrive at the equation for SHM. The constants A, ω, and φ depend on the specific characteristics of the spring and the mass attached to it.

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