Model Damped Harmonic Motion with Y=(e^ax) Sin/Cos bx

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Damped harmonic motion can be modeled using functions like y=(e^ax)sin(bx) or y=(e^ax)cos(bx), particularly in systems such as a mass on a spring or a simple pendulum. For effective damping, a "dashpot" is required to create resistance in the system. The underdamped case is particularly relevant, where the motion oscillates with decreasing amplitude over time. The resulting graph typically resembles y=(Ae^-ax)cos(bx+phi), illustrating the decay of oscillation. Understanding these concepts can help visualize and analyze real-world applications of damped motion.
botty_12
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Hey guys, using my knowledge of y=(e^ax) sin bx and y=(e^ax) cos bx, I need to find an example where these functions could be used as a model. I was thinking about damped harmonic motion but had a tough time trying to find an example and how i could relate it to those two graphs, any ideas?
 
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The example can be a simple pendulum. But "y" cannot be the two things simultaneously. It is sin or cos or more general: cos(bx+phi)
 
Would i be able to use a mass on the end of a spring? what would the graph look like if so?
 
Damped motion on a spring, voltage across an RC oscillator, an electromagnetic plane wave propagating through a lossy (or gain) medium, the tail of the wavefunction of a particle in a finite well: the list goes on and on and on.
 
Could i please have a quick explanation of the damped motion on a spring, and will the graph have a formula something like y=(Ae^-ax) cox (bx+pi)
 
Try wikipedia
 
botty_12 said:
Would i be able to use a mass on the end of a spring? what would the graph look like if so?

you'ld need a "dashpot" for there to be any damping.
 
Look for the underdampening case in damped harmonic motion.
 

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