Conservation of energy using a spring

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Homework Help Overview

The problem involves a 785-gram metal block on a table connected to a spring, exploring the conservation of energy as the block slides off the table. The block's motion is influenced by the spring's potential energy, kinetic energy, and friction, with specific values provided for the spring constant and friction coefficient.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss equating potential energy of the spring to kinetic energy of the block, while questioning the plausibility of the resulting distance. Some suggest using conservation of energy principles to analyze the motion from the table to the ground. Others emphasize the need to consider total energy changes, including gravitational potential energy.

Discussion Status

Participants are actively exploring different approaches to the problem, with some guidance offered on using conservation of energy. There is recognition of the need to account for various forms of energy and forces acting on the block. One participant expresses confusion about the force of friction but later indicates they resolved their misunderstanding.

Contextual Notes

There is a mention of the height of the table and the final velocity of the block, which are critical to the energy calculations. The discussion includes considerations of kinetic friction and its role in the energy balance.

rwinge
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Homework Statement



A 785-gram metal block is placed on a level table that is 1.6 m high. It is connected to a horizontal spring whose force constant is 3000 N/m. The block is pushed against the spring, compressing it by 0.100 m, and released. It slides along the table and goes off of the edge.

Coefficient of kinetic friction is 0.200 (Uk)

If the speed of the block just before it strikes the ground is 7.3 m/s, what distance did the block slide along the table?


Homework Equations



Work = delta K + delta U
U spring= (1/2)Kx^2
K block = (1/2)mv^2





The Attempt at a Solution



What I can come up with so far is that the potential energy of the spring (U) is equal to the kinetic energy done on the block (K). So in that case I set the two equations equal to each other

(1/2)Kx^2 = (Uk)mg(delta X) and so

15 J = 1.54(delta X)

so delta X = 9.74 m.


This doesn't seem very plausable to me with such a high spring coefficient and neglecting to use the height of the table and final velocity.

Any ideas?
 
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Start backwards. Use conservation of energy between the instant it leaves the table to the instant it hits the ground to solve for its speed as it left the table. Then use your work energy equation between the start point and the point it left the table.
 
You're assuming that the block goes only on the table. You need to take into account its total energy when compressed and its total energy when hitting the ground.
 
Last edited:
Okay so I think I am heading in the right direction now.

IVe got

Work = (delta K) + ( delta Uspring) + (delta Ugravity)

delta K = (1/2)Mvf^2 - (1/2)Mvi^2 = 20.92 J
delta Uspring = (1/2)Kxf^2 - (1/2)Kxi^2 = -15 J
delta Ugravity = (1/2)mghf - (1/2)kxf^2 = -12.31 J

adding theses gives me W = -6.39

I can also say that Wother = (coefficient of kinetic friction)(force of kinetic friction)(delta X)

in this case how am I coming up with the force of kinetic friction? because isn't that (coefficient of kinetic friction)*(normal force)? This just seems redundant to me.

any ideas?
 
Nevermind! haha I ended up getting it. I was just thinking about the force of friction wrong. Somehow I neglected to include gravity in my first calculation which gave an extremely long distance. thanks for the input guys!
 

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