Simple Harmonic Motion Reference Circle

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SUMMARY

This discussion focuses on calculating the position of an object undergoing simple harmonic motion (SHM) on a trampoline, specifically Ivan's oscillation with a period of 0.85 seconds and a maximum displacement of 0.14 meters. The reference circle method is employed, where the displacement after 1/8th of a cycle is derived using the formula y = a sin(θ), with θ being π/4 radians. The calculation confirms that the displacement is y = 0.14 sin(π/4) meters, emphasizing the importance of using radians in calculations.

PREREQUISITES
  • Understanding of simple harmonic motion (SHM)
  • Familiarity with trigonometric functions and their applications
  • Knowledge of reference circles in physics
  • Ability to convert between degrees and radians
NEXT STEPS
  • Explore the derivation of SHM equations using reference circles
  • Learn about angular velocity and its role in SHM
  • Study the effects of varying amplitude on SHM displacement
  • Investigate the relationship between period and frequency in oscillatory motion
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Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators looking for practical examples of simple harmonic motion concepts.

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Homework Statement


Through simple harmonic motion produced on a trampoline Ivan ossilates freely, with a period of 0.85s.
On a reference circle show Ivans position after 1/8th of a cycle. Label (and solve) the distance of this position from the equilibrium position.(Max displacement is 0.14m). C and A are labelled as the maximum displacement, and B the equilibrium position


Homework Equations





The Attempt at a Solution



I drew a reference circle, creating a right-angled triangle with an angle to the vertical of 45 degrees. The answer does not make much sense to me. Ill submit it as an attachment.
 

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When one uses a reference circle to derive the SHM equations it is assumed that the radius vector rotates at a constant angular velocity [tex]\omega[/tex]. Usually one takes it to rotate anticlockwise from some reference line. If the reference line is the horizontal line running through the diameter of the reference circle one would start the time measurement when the radius vector passes the three o'clock position. This would then give the formula

[tex]y = a \sin(\theta)[/tex]

for the displacement where [tex]theta[/tex] is the angle that the radius vector is making with the reference line. If one chooses to start the time measurement when the radius vector is at the twelve o'clock position the formula would use the cosine rather than the sine of the angle (which is then measured from the y-axis). In this case a is the amplitude of the motion which is 0.14 m.

For a complete cycle we have that

[tex]\theta = 2 \pi[/tex]

radians which means that for one eight of a cycle the angle would be

[tex]\theta = \frac{\pi}{4}[/tex]

radians which is [tex]45^o[/tex]

which means that the displacement would be

[tex]y = 0.14\sin(\frac{\pi}{4})[/tex]

meters after one eight of a cycle.
 
Last edited:
Important: should'n forget to position your calculator mode in radians, since equation deals with angular displacement theta in radians.
 

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