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The value of maximum possible amplitude in the case of forced oscillations when driving frequency is close to natural frequency is
  • A$\frac{{{F_0}}}{{m\,\left( {{\omega ^2}\, - \,\,\omega _d^2} \right)}}$
  • B$\frac{{{F_0}}}{{{\omega _d}b}}$
  • C$\frac{{{F_0}}}{{{m\omega ^2}}}$
  • D
    None
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