Calculating Velocity in Simple Harmonic Motion: A Homework Problem

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SUMMARY

The discussion centers on calculating the velocity of a rider on a mechanical bull undergoing simple harmonic motion (SHM) with an amplitude of 2.13 m and a frequency of 0.385 Hz. The relevant equations include V(ox) = -ωA sin(φ) and Vmax = ωAmplitude. The confusion arises around the phase angle and the relationship between the bull's acceleration and gravitational acceleration at the moment the rider leaves the saddle. The correct approach involves determining the bull's velocity when its downward acceleration exceeds that of gravity.

PREREQUISITES
  • Understanding of simple harmonic motion (SHM) principles
  • Familiarity with angular frequency calculations
  • Knowledge of the relationship between velocity, amplitude, and frequency in SHM
  • Basic grasp of gravitational acceleration effects on motion
NEXT STEPS
  • Study the derivation and application of the SHM velocity equation v = -A ω sin(ωt)
  • Learn about the concept of phase angle in oscillatory motion
  • Investigate the conditions under which an object in SHM can exceed gravitational acceleration
  • Explore practical applications of SHM in mechanical systems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators looking for examples of SHM applications in real-world scenarios.

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Homework Statement



While visiting friends at Cal State Chico, you pay a visit to the Crazy Horse Saloon. This fine establishment features a 200- kg mechanical bucking bull that has a mechanism that makes it move vertically in simple harmonic motion. Whether the “bull” has a rider or not, it moves with the same amplitude 2.13 m and frequency 0.385 Hz. Being from Texas you decide to ride it the “macho” way by NOT holding on. To no ones surprise you go flying out of the saddle. While waiting for your bruises and pride to heal, you decide to calculate how fast upward you were moving when you left the saddle.

Homework Equations



V(ox) = -\varpi*A*sin\phi

The Attempt at a Solution



I notice it is a simple harmonic motion question so I am using the equation relative to SRH velocities. Since it is a vertical motion, the gravity and mass play a role in the velocity. The angle I understand to be zero degrees?

I first found angular frequency by taking 2*pi*frequency. Then multiplied it by amplitude to get 5.15. The answer is 3.18. I know there is something small I'm missing, probably the mass factor, but I've been stuck for a while and could use some help...
 
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What angle?

Do you understand what that equation means?
 
The equation assumes t = 0 and v(ox) = v(x). I figured the initial velocity would be the instant the rider left the bull. the angle is the phase angle, and without an x direction, I didn't think there would be any angle. and since amplitude and frequency were given, that left me only a V(ox) variable to calculate.

I also tried to use:

Vmax = \varpi*Amplitude, from which I was initially under the impression was the correct way to do it but I am not returned close to the correct answer
 
Sounds like you're confused about what a "phase angle" is. The real equation is
v = -A \omega\,\mathrm{sin}(\omega t)
The \phi in your equation is equal to \omega t - it increases with time. It's not a real angle in space.

Now, think about what happens when you leave the bull flying upward: it means that the acceleration of gravity is not strong enough to hold you down to the bull. In other words, the bull would be accelerating downwards faster than the acceleration of gravity. Figure out how fast the bull is moving when that condition is met, and I think you'll have your answer.
 
I think I am confused about "phase angles" as well.

Figure out how fast the bull is moving once it exceeds the acceleration of gravity?
Does that mean I am still using the SHM veloctiy and acceleration equations?
 

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