Recent content by linyen416

  1. L

    Critical damping provides the quickest approach to zero amplitude

    theoretically it never reaches zero because of the exponential nature of decay, right?
  2. L

    Critical damping provides the quickest approach to zero amplitude

    wouldn't there be steady state errors in underdamped oscillation that is unforced?
  3. L

    Critical damping provides the quickest approach to zero amplitude

    cyrus, i was asking abotu unforced underdamped oscillation... so in actual physical systems they do reach zero and but theoretically they dont
  4. L

    Critical damping provides the quickest approach to zero amplitude

    So for an unforced underdamped oscillation, due to steady state errors that occur in real life, won't decay to zero?
  5. L

    Critical damping provides the quickest approach to zero amplitude

    cyrus, i thought damping brings it down to zero faster. also another thing that's troubling me is : for underdamping, overdamping, adn critical damping, do the amplitudes eventually REACH zero IN THEORY or is it that theoretically they only APPROACH zero? thanks
  6. L

    Critical damping provides the quickest approach to zero amplitude

    Critical damping provides the quickest approach to zero amplitude for a damped oscillator. With less damping (underdamping) it approaches zero displacement faster, but oscillates around it. With more damping (overdamping), the approach to zero is slower. I got this from hyperphysics but I...
  7. L

    Will a SHM eventually reach zero displacement or not?

    mgb, thanks for ur input! im wondering about underdamped oscillation as well. would displacement theoretically ONLY APPROACH zero?
  8. L

    Will a SHM eventually reach zero displacement or not?

    THEORETICALLY will a SHM eventually reach zero displacemtn or not? If it is DAMPED, amplitude would decrease with time, as would frequency, but would they would reach zero wouldn't they?
  9. L

    Exploring Forces in SHM: F=-kx & Weight's Impact

    so to clear things up: F = -kx refers to restorative force from springs F = -bv refers to the air resistance as the glider moves along and so if we use our amplitude -time graphs to calculated b, we should find that as m increases, b increases because the non-closed system causes extra...
  10. L

    Exploring Forces in SHM: F=-kx & Weight's Impact

    so I shouldn't explain the 'unlcosed-system' quality by saying that the wt force acts in a different vector componenet as the force from springs, but rather I should explain it by saying that the friction is introduced by the weight pushing down, so it's not exactly closed?
  11. L

    Exploring Forces in SHM: F=-kx & Weight's Impact

    SHM --> F = -kx SHM assumes that F is the only force acting on the system, so if we have a mass held between two springs on a linear air track, the F = -kx force refers to the restoring force from the springs? Is that the only thing it refers to? What about air resistance as the gliding...
  12. L

    Simple Harmonic Motion: Mass on a spring

    do you mean that F = -kx only applies before the spring moves? because I've measured spring constants by plotting Force vs. elongation graphs where force = mass hanging from spring *9.8 is that correct
  13. L

    Simple Harmonic Motion: Mass on a spring

    hi astronuc, i still don't understand why it's 2mg
  14. L

    SPRING CONSTANT- simple harmonic motion

    unless there's an equation that relates the individual spring constants to the effective spring constant when the mass is held between two identical springs
  15. L

    SPRING CONSTANT- simple harmonic motion

    So I think one way to get the effective spring constant is to use a pulley somehow.
Back
Top