Change in Amplitude with respect to Driven Frequencies

AI Thread Summary
The discussion focuses on analyzing the amplitude of a mass-spring system when driven at frequencies slightly above and below its natural frequency, ω0. The amplitude calculations involve using the provided equations, particularly how the damping constant affects the amplitude at different driving frequencies. The user attempts to derive the amplitude for a driving frequency of 10% above and below ω0, encountering a rounding error in their calculations. Clarifications are made regarding the distinction between natural frequency (ω0) and driving frequency (ωd) in the amplitude formula. The conversation emphasizes the importance of correctly identifying these frequencies in the context of the system's response.
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Homework Statement



A mass-spring system has b/m = \omega_0/5 , where b is the damping constant and \omega_0 the natural frequency. How does its amplitude when driven at frequencies 10% above \omega_0 compare with its amplitude at \omega _0 ? How does its amplitude when driven at frequencies 10% below \omega_0 compare with its amplitude at \omega _0 ?

Homework Equations



(1) A(\omega) = \frac{F_0}{m\sqrt{(\omega^2_d - \omega^2_0)^2 + \frac{b^2\omega^2_0}{m^2}}}

(2) \omega^2_0=\frac{25b^2}{m^2}

The Attempt at a Solution



Plugging in 1.1 for \omega_d in equation 1 (since it is 10% more than \omega_0 ) and using equation 2 to substitute \omega^2_0 for \frac{25b^2}{m^2} gives an amplitude of \frac{mF_0}{b^2}*1/7.25 . Plugging in 0 for the driving force yields an amplitude of \frac{mF_0}{b^2}*1/5 . The amplitude when driven over the amplitude given by the natural frequency should be 5/7.25*100%. Rounded to two sig figs, as my online homework demands, should yield 69%. It is telling me that I have made a rounding error, but I cannot find where.
 
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\omega_0 should not change whether the system is driven or not. It is the natural frequency. \omega_d however, will be changing in each of the three calculations of amplitude.
 
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