Dynamic Magnification Factor is computed as:
the ratio of the maximum dynamic deflection to the maximum static deflection.
The Dynamic Magnification Factor (DMF) is a crucial concept in structural dynamics. It helps us understand how much larger the deflection or stress in a structure under a dynamic load is compared to the deflection or stress it would experience under the same load applied statically.
Let's consider a dynamic load acting on a structure. This load can cause oscillations and potentially larger deflections than if the load were applied slowly and gradually (statically).
The Dynamic Magnification Factor quantifies this effect. It is defined as the ratio of the maximum dynamic deflection observed under the dynamic load to the maximum static deflection that would occur if the same load were applied statically.
Mathematically, the Dynamic Magnification Factor (DMF) is expressed as:
\text{DMF} = \frac{\text{Maximum Dynamic Deflection}}{\text{Maximum Static Deflection}}
Let's look at the given options in light of this definition:
Therefore, the correct way to compute the Dynamic Magnification Factor is by taking the ratio of the maximum dynamic deflection to the maximum static deflection.
When ω/ωn = 1, the transmissibility is
where ω = frequency of excitation, rad/s
ωn = Natural frequency, rad/s
The Transmissibility of a vibrating system, for the values of (ω/ωn) >√2, will be
A vibrating system having a mass of 30 kg is supported by 4 springs, each having a stiffness of k. The system runs at 420 rpm. If only 10% of the shaking force is allowed to be transmitted to the supporting structure, then the value of stiffness k will be close to:
For a single degree of freedom viscous damped system, if the frequency ratio is greater than √2, it implies that:
A single degree of freedom system having mass 1 kg and stiffness 10 kN/m initially at rest is subjected to an impulse force of magnitude 5 kN for 10-4 seconds. The amplitude in mm of the resulting free vibration is