Conservation of energy with spring

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SUMMARY

The discussion focuses on the conservation of energy principles applied to a mass-spring system. A spring with a constant of 22 N/m is compressed by a 0.4 kg mass and then released, skidding over a frictional surface with a coefficient of friction of 0.17 before compressing a second spring with a constant of 2 N/cm. The key equations used include the work-energy principle and the relationship between kinetic energy and potential energy. The challenge lies in calculating how far the second spring compresses to bring the mass to a stop, factoring in the work done by friction.

PREREQUISITES
  • Understanding of Hooke's Law and spring constants
  • Familiarity with the work-energy theorem
  • Knowledge of kinetic and potential energy equations
  • Basic concepts of friction and its coefficients
NEXT STEPS
  • Calculate the work done by friction using W = Fd
  • Learn how to apply the work-energy principle to mass-spring systems
  • Explore the effects of different spring constants on energy conservation
  • Investigate the relationship between kinetic energy and spring compression
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Physics students, mechanical engineers, and anyone interested in understanding energy conservation in mechanical systems.

fanie1031
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1. A spring of constant 22 N/m is compressed a distance 8 cm by a 0.4kg mass, then released. It skids over a frictional surface of length 2.3m with coefficient of friction 0.17, then compresses the second spring of constant 2N/cm. The acceleration of gravity is 9.8m/s(squared). How far will the second spring cmpress in order to bring the mass to a stop? Answer in cm.



2.

W=Fd
.5mgyf + .5Kdelta(X squared) = .5mgyo + .5Kdelta(Xsquared)
also mgyf + 1/2mVf^2 = mgyo + 1/2mVo^2




3. I used all three formulas but the fact that I'm using cefficients is throwing me off.
 
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Hi fanie1031,

fanie1031 said:
1. A spring of constant 22 N/m is compressed a distance 8 cm by a 0.4kg mass, then released. It skids over a frictional surface of length 2.3m with coefficient of friction 0.17, then compresses the second spring of constant 2N/cm. The acceleration of gravity is 9.8m/s(squared). How far will the second spring cmpress in order to bring the mass to a stop? Answer in cm.



2.

W=Fd


For consant forces the work done is:

<br /> W=F d \cos\theta<br />
where theta is the angle between the force and the displacement of the object. What would theta be for the work done by this frictional force? What would F and d be?



.5mgyf + .5Kdelta(X squared) = .5mgyo + .5Kdelta(Xsquared)
also mgyf + 1/2mVf^2 = mgyo + 1/2mVo^2

These two formulas do not apply to this problem. A good starting point for these problems is:

<br /> W_{\rm nc} = E_f - E_i<br />

which means

(work done by non-conservative forces during displacement) = (energy at end of displacement) - (energy at beginning of displacement)


What does this give?
 

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