Calculating Amplitude and Phase for Superimposed Harmonic Oscillators

In summary, the question involves finding the amplitude and phase of a superimposed oscillation of two simple harmonic oscillators with different amplitudes and a phase difference of 30°. To better understand the concept, manually graphing the waves and adding their amplitudes may be helpful.
  • #1
kidia
66
0
Can anybody give me the hint where to start on this question?

Two simple harmonic oscillators of the same frequency and in the same direction having amplitudes 5 mm and 3 mm, respectively and the phase of the second component relative to the first is 30°, are superimposed. Find the amplitude of the resultant oscillation and its phase relative to the first component.
 
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  • #2
Whether or not it will suffice as "properly done," try manually graphing these waves on graph paper (two cycles of each wave, max), and adding their amplitudes to find the superimposed amplitude. It will give you insight to what is going on.

If you need to show the math, begin by finding the expression for amplitude for each wave as a funtion of wt.
 
  • #3


To calculate the amplitude and phase for superimposed harmonic oscillators, we first need to understand the concept of superposition. Superposition is the principle that states that when two or more waves or oscillations are combined, the resulting wave is the sum of the individual waves.

In this case, we have two simple harmonic oscillators with the same frequency and direction but different amplitudes and a phase difference of 30°. To find the amplitude of the resultant oscillation, we can use the formula A = √(A1^2 + A2^2 + 2A1A2cosϕ), where A1 and A2 are the amplitudes of the individual oscillators and ϕ is the phase difference between them.

Substituting the given values, we get A = √(5^2 + 3^2 + 2(5)(3)cos30°) = √(25 + 9 + 30) = √64 = 8 mm.

To find the phase of the resultant oscillation relative to the first component, we can use the formula tanϕ = (A2sinϕ)/(A1 + A2cosϕ). Substituting the given values, we get tanϕ = (3sin30°)/(5 + 3cos30°) = 0.5/6.5 = 0.0769. Taking the inverse tangent, we get ϕ = 4.4°.

Therefore, the amplitude of the resultant oscillation is 8 mm and its phase relative to the first component is 4.4°. This means that the resulting oscillation will have an amplitude of 8 mm and will be shifted by 4.4° in the direction of the second component.
 

What is a simple harmonic oscillator?

A simple harmonic oscillator is a physical system that exhibits a repeating, oscillating motion about a stable equilibrium point. It follows the principle of Hooke's Law, which states that the restoring force of an object is directly proportional to its displacement from its equilibrium position.

What are some examples of simple harmonic oscillators?

Some examples of simple harmonic oscillators include a mass-spring system, a pendulum, and a vibrating guitar string. These systems all have a restoring force that is proportional to their displacement from equilibrium, allowing them to exhibit harmonic motion.

What is the equation for the motion of a simple harmonic oscillator?

The equation for the motion of a simple harmonic oscillator can be written as x(t) = A cos(ωt + φ), where x is the displacement from equilibrium, A is the amplitude of the oscillation, ω is the angular frequency, and φ is the phase angle. This equation describes a sinusoidal motion with a constant amplitude and frequency.

What affects the period and frequency of a simple harmonic oscillator?

The period and frequency of a simple harmonic oscillator are affected by the mass of the object, the spring constant, and the amplitude of the oscillation. The period is directly proportional to the mass and the square root of the spring constant, while the frequency is inversely proportional to these factors.

How is the energy of a simple harmonic oscillator related to its motion?

A simple harmonic oscillator has both kinetic and potential energy, which alternate between each other as the object moves. The total energy of the oscillator is constant and is equal to the sum of its kinetic and potential energies. As the amplitude of the motion decreases, the energy is transferred back and forth between the two forms, resulting in a decrease in amplitude over time.

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