How Do You Determine Spring Compression in Harmonic Motion?

In summary, the speed of the 2 kg block at the instant it hits the end of the spring is 2.970 m/s and the period of the simple harmonic motion that ensues is 0.628 seconds. The distance that the spring is compressed at the instant the speed of the block is maximum is either zero if the block is at its maximum speed just as it hits the spring, or can be calculated by equating the kinetic energy of the block before impact to the work done in compressing the spring if the word "maximum" should read "minimum".
  • #1
zbirdie
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Homework Statement



A 2 kg block is dropped from a height of .45 m above an uncompressed spring. The springs k value is 200 N/m, and has negligible mass. The block strikes the end of the spring and sticks to it.

a) determine the speed of the block at the instant it hits the end of the spring.

Ok, I did this, I am fairly certain my answer is correct, because I checked it using conservation of energy. Anyhow, I got that the speed of the block at the instant it hits the end of the spring was V=2.970 m/s

b) Determine the period of the simple harmonic motion that ensues.

OK, did this, using the equation for Ts, and got that T=.628s.

c) Determine the distance that the spring is co0mpressed at the instant the speed of the block is maximum.

Ok, this is the part where I need help. I want to use conservation of energy, and I know that I can, because although the spring and the block collide, the spring is massless, so no heat is created.

The relevant equation for this part is (I think) Vmax=wwA. For w, I plugged in 2pi/T=10rad/s. Then for Vmax I used 2.970m/s. This is the main part I am having doubts about. My logic was that since this is the velocity right when the block hits the uncompressed spring, there is no SPE, so there fore the velocity is the maximum it could ever be. Anyways, using this method, I got that the amplitude, and thus the compression of the spring at the highest velocity of the block, was .03m, or 3cm. I don't know if this is right, so I would greatly appreciate reassurance/guidance on how to do this correctly. Thank you
 
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  • #2
c) Determine the distance that the spring is co0mpressed at the instant the speed of the block is maximum.

Surely the block is at its maximum speed just as it hits the top of the spring and therefore the compression is zero.

If on the other hand the word "maximum" should read "minimum", then its just a question of equating the kinetic energy of the block before impact to the work done (i.e. force * distance) compressing the spring to halt the block.
 
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  • #3
.I would like to commend you on your thorough understanding and application of conservation of energy in solving parts a) and b) of this problem. Your calculation for the speed of the block at the instant it hits the end of the spring seems correct, and your approach for determining the period of the simple harmonic motion is also correct.

For part c), your logic is sound in using conservation of energy to determine the amplitude of the spring. However, there are a few things to consider. Firstly, the equation you used, Vmax=wwA, is actually the equation for the maximum speed of an object undergoing simple harmonic motion, not the amplitude. The amplitude, A, can be found by rearranging this equation to A=Vmax/(ww). Secondly, you used the value of 2.970 m/s for Vmax, which is actually the speed of the block at the instant it hits the end of the spring. This is not the maximum speed of the block during the entire motion, as the block will eventually come to a stop and reverse direction. The maximum speed of the block during this motion can be found by using the equation Vmax=Aw, where w is the angular frequency, which you correctly calculated to be 10 rad/s. Substituting these values into the equation, we get Vmax=0.03 m/s. This is the maximum speed of the block during the motion, which occurs at the equilibrium position of the spring. Since the block is at maximum speed at this point, it means that all of its initial potential energy has been converted into kinetic energy. Therefore, the amplitude of the spring at this point is equal to the maximum compression of the spring, which is 0.03 m or 3 cm.

In summary, your approach was correct, but there were some minor errors in the equations and values used. Keep up the good work and continue to apply your understanding of conservation of energy in solving problems like these.
 

FAQ: How Do You Determine Spring Compression in Harmonic Motion?

What is a vertical spring pendulum?

A vertical spring pendulum is a physical system consisting of a mass attached to a spring and allowed to oscillate in a vertical direction. The spring is fixed at one end while the other end is attached to the mass, creating a pendulum-like motion.

What factors affect the motion of a vertical spring pendulum?

The motion of a vertical spring pendulum is affected by the mass of the object, the length of the spring, and the strength of the spring. Other factors such as air resistance and friction can also have an impact on the motion.

How does the amplitude of a vertical spring pendulum change over time?

The amplitude of a vertical spring pendulum decreases over time due to the effects of damping. Damping is the gradual loss of energy from the system, causing the amplitude to decrease until the pendulum eventually comes to a stop.

Can the motion of a vertical spring pendulum be described mathematically?

Yes, the motion of a vertical spring pendulum can be described using mathematical equations such as Hooke's law, which relates the force exerted by the spring to its displacement. The equations of motion can also be used to determine the period and frequency of the pendulum's oscillations.

What are the practical applications of a vertical spring pendulum?

A vertical spring pendulum has various practical applications, such as in shock absorbers for vehicles and buildings, as well as in various scientific experiments to study harmonic motion and energy transfer. It can also be used as a toy or educational tool to demonstrate the principles of oscillation and wave motion.

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