Simple Harmonic Motion of an oscillating particle

In summary, given an oscillating particle with a period of 56 s and an amplitude of 18 cm, the distances traveled during the following intervals are: (a) 18 cm, (b) 0 cm, (c) 9 cm, (d) 9 cm. This can be found by using the equation x = Acos(\omega * t * \delta) and substituting the values for \omega and \delta, and then calculating for each interval.
  • #1
maniacp08
115
0
The period of an oscillating particle is 56 s, and its amplitude is 18 cm. At t = 0, it is at its equilibrium position. Find the distances traveled during these intervals.
(a) t = 0 to t = 14 s
cm

(b) t = 14 s to t = 28 s
cm

(c) t = 0 to t = 7 s
cm

(d) t = 7 s to t = 14 s
cm

x = Acos([tex]\omega[/tex] * t * [tex]\delta[/tex])
[tex]\omega[/tex] = 2[tex]\pi[/tex] / T
[tex]\omega[/tex] = 2[tex]\pi[/tex] / 56

Since x = 0 when t = 0
Then [tex]\delta[/tex] = [tex]\pi[/tex] / 2
correct?

for part A)

x = 18cm * cos[2[tex]\pi[/tex] / 56 * 14s + [tex]\pi[/tex] / 2] - cos[2[tex]\pi[/tex] / 56 * 0s + [tex]\pi[/tex] / 2]

Is this good?
 
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  • #2
Hi maniacp08,

maniacp08 said:
The period of an oscillating particle is 56 s, and its amplitude is 18 cm. At t = 0, it is at its equilibrium position. Find the distances traveled during these intervals.
(a) t = 0 to t = 14 s
cm

(b) t = 14 s to t = 28 s
cm

(c) t = 0 to t = 7 s
cm

(d) t = 7 s to t = 14 s
cm

x = Acos([tex]\omega[/tex] * t * [tex]\delta[/tex])
[tex]\omega[/tex] = 2[tex]\pi[/tex] / T
[tex]\omega[/tex] = 2[tex]\pi[/tex] / 56

Since x = 0 when t = 0
Then [tex]\delta[/tex] = [tex]\pi[/tex] / 2
correct?

for part A)

x = 18cm * cos[2[tex]\pi[/tex] / 56 * 14s + [tex]\pi[/tex] / 2] - cos[2[tex]\pi[/tex] / 56 * 0s + [tex]\pi[/tex] / 2]

The 18cm needs to multiply both cosine functions, not just the first one. Was that just a typo?

Also you can think about how the time period of 14 seconds is related to the period, to get the answer right away.
 
  • #3


Yes, your approach is correct. Here is a breakdown of the steps for each part:

(a) t = 0 to t = 14 s
To find the distance traveled during this interval, we can use the formula x = Acos(\omega * t), where A is the amplitude and \omega is the angular frequency. Plugging in the given values, we have x = 18cm * cos[(2\pi / 56) * 14s]. This simplifies to x = 18cm * cos(0.5\pi) = 18cm * 0 = 0cm. Therefore, the particle does not travel any distance during this interval as it remains at its equilibrium position.

(b) t = 14 s to t = 28 s
Using the same formula, we have x = 18cm * cos[(2\pi / 56) * 28s]. This simplifies to x = 18cm * cos(\pi) = 18cm * (-1) = -18cm. Therefore, the particle travels a distance of 18cm to the left during this interval.

(c) t = 0 to t = 7 s
Using the formula x = Acos(\omega * t), we have x = 18cm * cos[(2\pi / 56) * 7s]. This simplifies to x = 18cm * cos(0.25\pi) = 18cm * 0.7071 = 12.73cm. Therefore, the particle travels a distance of 12.73cm to the right during this interval.

(d) t = 7 s to t = 14 s
Using the same formula, we have x = 18cm * cos[(2\pi / 56) * 14s] - 18cm * cos[(2\pi / 56) * 7s]. This simplifies to x = 18cm * cos(0.5\pi) - 18cm * cos(0.25\pi) = 0cm - 12.73cm = -12.73cm. Therefore, the particle travels a distance of 12.73cm to the left during this interval.
 

1) What is Simple Harmonic Motion (SHM)?

Simple Harmonic Motion refers to the repetitive motion of an oscillating particle that follows a sinusoidal pattern. This means that the displacement of the particle from its rest position is directly proportional to the force acting on it and is in the opposite direction of the displacement.

2) What are the key characteristics of SHM?

The key characteristics of SHM are amplitude, frequency, and period. Amplitude is the maximum displacement of the particle from its rest position, frequency is the number of oscillations per unit time, and period is the time it takes for one complete oscillation.

3) What is the equation for Simple Harmonic Motion?

The equation for Simple Harmonic Motion is x = A*sin(ωt + φ), where x is the displacement of the particle, A is the amplitude, ω is the angular frequency, and φ is the phase constant.

4) How does SHM relate to real-life phenomena?

SHM can be observed in several real-life phenomena, such as the motion of a pendulum, a mass-spring system, and even sound waves. It is a fundamental concept in physics and can help explain the behavior of various systems and objects.

5) What factors affect the period and frequency of SHM?

The period and frequency of SHM are affected by the mass of the oscillating particle, the force acting on it, and the stiffness of the system. An increase in mass or stiffness leads to a longer period and a lower frequency, while an increase in force will result in a shorter period and a higher frequency.

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