Change in Amplitude with respect to Driven Frequencies

In summary, when a mass-spring system is driven at frequencies 10% above its natural frequency, the amplitude is reduced by approximately 31%, while when driven at frequencies 10% below its natural frequency, the amplitude is increased by approximately 25%. This is based on the equations A(\omega) = \frac{F_0}{m\sqrt{(\omega^2_d - \omega^2_0)^2 + \frac{b^2\omega^2_0}{m^2}}} and \omega^2_0=\frac{25b^2}{m^2}. The natural frequency, \omega_0, remains constant, while the driving frequency, \omega_d, changes.
  • #1
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Homework Statement



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

Homework Equations



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

(2) [tex] \omega^2_0=\frac{25b^2}{m^2} [/tex]

The Attempt at a Solution



Plugging in 1.1 for [tex] \omega_d [/tex] in equation 1 (since it is 10% more than [tex] \omega_0 [/tex] ) and using equation 2 to substitute [tex] \omega^2_0 [/tex] for [tex] \frac{25b^2}{m^2} [/tex] gives an amplitude of [tex] \frac{mF_0}{b^2}*1/7.25 [/tex] . Plugging in 0 for the driving force yields an amplitude of [tex] \frac{mF_0}{b^2}*1/5 [/tex] . 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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  • #3
[tex] \omega_0 [/tex] should not change whether the system is driven or not. It is the natural frequency. [tex] \omega_d [/tex] however, will be changing in each of the three calculations of amplitude.
 

What is meant by "change in amplitude with respect to driven frequencies"?

The change in amplitude with respect to driven frequencies refers to how the amplitude, or strength, of a wave changes when it is driven by an external force at different frequencies. This change can be observed in many types of waves, including sound waves and electromagnetic waves.

How does the amplitude change with respect to driven frequencies?

The amplitude of a wave typically increases as the driving frequency approaches the natural frequency of the system. This is known as resonance. However, as the driving frequency continues to increase, the amplitude will eventually decrease. This relationship is known as the amplitude-frequency response curve.

What factors affect the change in amplitude with respect to driven frequencies?

The change in amplitude with respect to driven frequencies is affected by the properties of the system being driven, such as its natural frequency and damping coefficient. It is also influenced by the frequency and strength of the driving force.

Why is understanding the change in amplitude with respect to driven frequencies important?

Understanding the change in amplitude with respect to driven frequencies is important in many fields of science and engineering. It can help predict how a system will respond to external forces and how to optimize its performance. It is also crucial in designing and troubleshooting systems that rely on resonance, such as musical instruments and electronic circuits.

How is the change in amplitude with respect to driven frequencies measured?

The change in amplitude with respect to driven frequencies can be measured using various techniques, such as Fourier analysis or a frequency response test. These methods allow for the visualization and analysis of the amplitude-frequency response curve, which can provide valuable information about the system being driven.

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