Plane polarized oscilation of a spring

In summary, the conversation discusses determining the energy of a spring with a given elastic constant, natural width, and mass, when it is put into oscillation with fixed ends. The frequency and amplitude of the oscillation are also mentioned, and it is noted that the frequency may be determined from the given constants. Additionally, it is clarified that the oscillation is a second harmonic sine function with one crest and one valley. The conversation ends with a request for help and well wishes.
  • #1
DaTario
1,056
39
Hi All,

Suppose you have a spring with a given elastic constant k. Its natural width is L = 1 meter and its mass is M = 0.1 kg. Now imagine you put this spring to oscilate, with its ends fixed, forming a pure second harmonic oscilation, plane polarized, with frequency Omega. The amplitude of this oscillation is A = 1 meter also.
How is one to determine the energy E of this system ? (mechanical energy of this system E = Ekin + Epot)

P.S. it seems natural that the frequency Omega is to be determined from the constants I alluded above.

P.S. 2: by second harmonic I mean a sine function between the end points (x = 0 and x = 1) with just one crest and one valley.

Best Regards

DaTario
 
Last edited:
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  • #2
Wait, be faithful, may be the help is to arrive soon...

Best Regards

DaTario
 
  • #3


Hello DaTario,

Thank you for your question! I would approach this problem by first considering the basic principles of energy in a system. In this case, the total energy of the system can be calculated as the sum of its kinetic energy (E_kin) and potential energy (E_pot).

To determine the kinetic energy, we need to know the mass of the spring and its velocity. Since the spring is undergoing a second harmonic oscillation, its velocity can be expressed as v = A*Omega*cos(Omega*t), where A is the amplitude and Omega is the frequency. Therefore, the kinetic energy can be calculated as E_kin = 0.5*M*(A*Omega*cos(Omega*t))^2.

Next, we need to determine the potential energy of the system. In this case, the potential energy is due to the elastic potential energy stored in the spring. This can be expressed as E_pot = 0.5*k*x^2, where k is the elastic constant and x is the displacement of the spring from its equilibrium position. Since the spring is undergoing a second harmonic oscillation, the displacement can be expressed as x = A*sin(Omega*t). Therefore, the potential energy can be calculated as E_pot = 0.5*k*(A*sin(Omega*t))^2.

Finally, we can calculate the total energy of the system by summing the kinetic and potential energies: E = E_kin + E_pot. By substituting the expressions we derived above, we get E = 0.5*M*(A*Omega*cos(Omega*t))^2 + 0.5*k*(A*sin(Omega*t))^2. This expression gives us the total energy of the system at any given time during the oscillation.

To find the frequency Omega of the oscillation, we can use the relationship between frequency, mass, and spring constant, which is given by Omega = sqrt(k/M). Therefore, by plugging in the values of k and M given in the problem, we can determine the frequency of the oscillation.

I hope this explanation helps you understand how to determine the energy of a system undergoing plane polarized oscillation of a spring. Let me know if you have any further questions. Best regards,
 

Related to Plane polarized oscilation of a spring

1. What is plane polarized oscillation of a spring?

Plane polarized oscillation of a spring is a type of motion that occurs when a spring is stretched or compressed in a single direction, resulting in a back and forth movement around a fixed point.

2. How is plane polarized oscillation different from other types of motion?

Unlike other types of motion, such as circular or elliptical motion, plane polarized oscillation is restricted to a single plane and has a constant amplitude and frequency.

3. What factors affect the plane polarized oscillation of a spring?

The main factors that affect plane polarized oscillation are the stiffness of the spring, the mass attached to the spring, and the amplitude and frequency of the oscillation.

4. How is plane polarized oscillation used in scientific research?

Plane polarized oscillation of a spring is used in various scientific experiments, such as studying the behavior of materials under stress or investigating the properties of waves and vibrations.

5. Can plane polarized oscillation be observed in everyday life?

Yes, plane polarized oscillation can be observed in everyday life, such as in the movement of a diving board or a swinging pendulum.

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