Question

A $50-\mathrm{kg}$ machine is mounted on four parallel springs, each of stiffness $3 \times 10^5 \mathrm{~N} / \mathrm{m}$. What is the maximum transmitted force when the machine is subject to an excitation of the form of Fig. 8-12 with $F_0=1200 \mathrm{~N}$ and $t_0=0.05 \mathrm{~s}$ ?

   A $50-\mathrm{kg}$ machine is mounted on four parallel springs, each of stiffness $3 \times 10^5 \mathrm{~N} / \mathrm{m}$. What is the maximum transmitted force when the machine is subject to an excitation of the form of Fig. 8-12 with $F_0=1200 \mathrm{~N}$ and $t_0=0.05 \mathrm{~s}$ ?
 
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Theory and problems of mechanical vibrations
Theory and problems of mechanical vibrations
S. Graham Kelly 1st Edition
Chapter 8, Problem 52 ↓

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The excitation function is of the form $F(t) = F_0 \sin(\omega t)$, where $F_0 = 1200 \mathrm{~N}$ and $t_0 = 0.05 \mathrm{~s}$. The maximum displacement can be found using the equation $x_{\text{max}} = \frac{F_0}{k}$, where $k$ is the stiffness of the spring.  Show more…

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A $50-\mathrm{kg}$ machine is mounted on four parallel springs, each of stiffness $3 \times 10^5 \mathrm{~N} / \mathrm{m}$. What is the maximum transmitted force when the machine is subject to an excitation of the form of Fig. 8-12 with $F_0=1200 \mathrm{~N}$ and $t_0=0.05 \mathrm{~s}$ ?
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Key Concepts

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Transient Force Excitation
Transient force excitations refer to forces that change rapidly over time, typically applied over a short duration. These forces can result in significant dynamic responses because the system does not have time to adjust gradually, potentially leading to high acceleration and amplified forces within the structure. Understanding transient excitations is essential in many engineering applications to design systems that can withstand sudden impacts or loads without failure.
Dynamic Force Amplification
Dynamic force amplification describes the phenomenon where the forces transmitted through a system under dynamic loading conditions can exceed the magnitude of the applied static load. This is due to the inertia of the mass and the timing of the load application relative to the system's natural frequency. Recognizing and calculating this amplification is vital in engineering design, as it ensures that supports and connections are robust enough to handle the peak forces that may occur during transient events.
Parallel Springs Equivalent Stiffness
When several springs are arranged in parallel, the effective stiffness of the system is obtained by summing the individual spring constants. This concept is fundamental because it allows one to simplify the analysis of complex support systems by replacing multiple springs with a single equivalent spring that has a stiffness equal to the sum of the component springs. Calculating the equivalent stiffness is crucial for evaluating how a structure will deform and how forces will be distributed across the supports under load.
Mass-Spring System Dynamics
A mass-spring system is a basic model used in dynamics to study how a mass responds to forces through elastic supports. The response of the system is characterized by parameters such as the natural frequency, which depends on the mass and the overall system stiffness. This concept is important because it determines how the system will vibrate when subjected to dynamic or transient loads, influencing both the amplitude and the phase of the response relative to the applied excitation.

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