Does logarithmic decrement depend on initial amplitude?

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Logarithmic decrement does not remain constant across different initial amplitudes when a weight is attached to a spring and released underwater. The relationship between amplitude and logarithmic decrement is influenced by the damping force, which may not be proportional to velocity in real-world scenarios. For instance, damping forces caused by fluid viscosity can vary with the square of the velocity, while frictional damping can be constant. The formula for logarithmic decrement is most accurate when the time interval aligns with the oscillation period. Therefore, the behavior of logarithmic decrement and the period of oscillation can change based on the specific damping conditions present.
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Lets say we have a weight attached to a spring. When releasing it under water (whole motion occours under water) at different initial amplitudes, will logarithmic decrement be the same? And will the period change?

I think it should be the same for different initial amplitudes. But \Theta=\frac{T_1}{t}\ln\frac{A_1}{A(t)}, where T_1 is period of first cycle, t is time until amplitude is A(t) and A_1 is initial amplitude, suggests that when initial amplitude increases, logarithmic decrement must increase as well, or the ratio \frac{T_1}{t} must decrease.

So... which one is correct?
 
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Your formula for log dec is only correct when the time interval is an exact multiple of the oscillation period.

In real life, you can use the formula approxiamately for any time interval, by drawing a smooth curve through the maximum amplitude of each cycle, and using that curve for the amplitudes "A" in the formula.

Also, the log dec is only constant if the damping force is proportional to velocity. That is the "standard" equation that you study for single degree of freedom damped systems, but in real life damping forces are often NOT proportional to velocity. For example the damping force caused by viscosity of a fluid (like your water example) is approximately proportional to velocity squared, except at very low velocities.

As another example, a frictional damping force that obeys Coulomb's law of friction is constant (indepdendent of velocity). For friction damping, the motion will stop completely after a finite number of oscillations, which can't happen with the log dec is constant.
 
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