Driven Oscillation: Springboard diving

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SUMMARY

The discussion centers on the physics of oscillation in a springboard diving scenario, specifically analyzing the amplitude and acceleration of a diver as he becomes airborne. The diver, weighing 65 kg, depresses the springboard by 25 cm, and the problem requires calculating the amplitude of oscillation and acceleration at the moment of takeoff. Key equations include the relationship between amplitude (A), frequency (f), spring constant (k), and mass (m), which are essential for solving the problem. The diver's motion is described as resonant with the oscillation of the board, raising questions about the potential for amplitude increase beyond the equilibrium position.

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  • Understanding of harmonic motion and oscillation principles
  • Familiarity with Hooke's Law and spring constants
  • Knowledge of basic calculus and physics equations related to motion
  • Ability to interpret and manipulate equations for frequency and amplitude
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  • Study the derivation of the spring constant (k) in oscillatory systems
  • Learn about resonance in mechanical systems and its effects on amplitude
  • Explore the mathematical proof of energy conservation in oscillating systems
  • Investigate the relationship between mass, spring constant, and frequency in depth
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Physics students, educators, and anyone interested in the mechanics of oscillation and resonance in spring systems, particularly in the context of sports science and engineering applications.

Beth N
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Homework Statement


A light springboard deflects 15cm when a 65kg diver stands on its end. He jumps up and down, depressing it by 25 cm, then he moves up and down with the oscillations of the end of the board.
What is the amplitude of the oscillation when the diver just become airborne? What is the acceleration at this point?
(in solving problem c, assuming that we have acquired the frequency and the maximum speed from question a and b)

Below is the problem. I highlighted in red the question I have. Feel free to skip uneccessary information.

Screen Shot 2018-10-07 at 11.44.25 AM.png
Screen Shot 2018-10-07 at 11.45.02 AM.png
Screen Shot 2018-10-07 at 11.51.12 AM.png

Homework Equations



##a=A * ( 2 \pi f)^2##

##v=\frac 1 2kA^2##

##f=\frac 1 2\pi (\sqrt {\frac k m})##
a is acceleration, A is amplitude, f is frequency, k is spring constant m is mass

The Attempt at a Solution


[/B]
The big question I have isn't exactly the question c in the problem, but: why we can be sure that the board won't bend beyond its undeflected position? My thought is that maybe there is no energy input, no force pointing upward; the only driving force here is the man's weight. So when the man no longer exert his weight force upon the board, there is no more restoring force by the board on the man opposing his weight. Hence the board return to its equilibrium position at 0 (in picture).

However, am I correct to say that the man is jumping up and down in resonance with the oscillation of the board? Could resonance possibly increase the amplitude beyond point 0? How can I prove this mathematically? (I tried using the equations I listed above but didn't succeed.
 

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Beth N said:
However, am I correct to say that the man is jumping up and down in resonance with the oscillation of the board?
The problem states that
Beth N said:
... he moves up and down with the oscillations of the end of the board.
This, to me, means that he is just at the threshold of losing contact at 5 cm below the position "zero" of the plank. Figure 14.30 shows the position of his feet and the plank at any time t. If he is launched in the air, yes the board will go above the zero point, but this is not what is described in the problem.
 

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