Vibrations are oscillatory motions of objects or systems around equilibrium positions. This unit covers key concepts like period, frequency, amplitude, and degrees of freedom. It explores different types of vibrations, including free, forced, damped, and undamped oscillations.
Mathematical models and equations are used to analyze vibrating systems. The mass-spring-damper model is introduced, along with equations of motion for single degree of freedom systems. Free and forced vibration analyses are covered, including natural frequencies, damping ratios, and resonance phenomena.
Key Concepts and Terminology
Vibration the oscillatory motion of a system or object around an equilibrium position
Period (T) time required for one complete cycle of oscillation, measured in seconds
Frequency (f) number of cycles per unit time, measured in Hertz (Hz) or cycles per second
Related to period by the equation f=T1
Amplitude maximum displacement from the equilibrium position during oscillation
Angular frequency (ω) measured in radians per second, related to frequency by ω=2πf
Degrees of freedom (DOF) number of independent coordinates needed to describe a system's motion
Single DOF systems have one coordinate (mass-spring system)
Multi DOF systems have multiple coordinates (coupled pendulums)
Natural frequency frequency at which a system oscillates when disturbed from its equilibrium position without external forces
Types of Vibrations
Free vibration occurs when a system oscillates without any external forces acting on it
Determined by the system's inherent properties (mass, stiffness, damping)
Forced vibration occurs when a system is subjected to an external force or excitation
Steady-state response depends on the frequency and amplitude of the external force
Undamped vibration oscillation without any energy dissipation, resulting in constant amplitude
Damped vibration oscillation with energy dissipation, causing the amplitude to decrease over time
Viscous damping force proportional to velocity (hydraulic shock absorbers)
Coulomb damping force constant in magnitude but opposite to the direction of motion (dry friction)
Linear vibration systems with linear restoring forces, resulting in sinusoidal motion
Nonlinear vibration systems with nonlinear restoring forces, leading to complex motion (hardening or softening springs)
Mathematical Models and Equations
Mass-spring-damper model simplest representation of a vibratory system
Consists of a mass (m), spring with stiffness (k), and damper with damping coefficient (c)
Equation of motion describes the system's dynamic behavior, derived using Newton's second law
For a single DOF system: mx¨+cx˙+kx=F(t), where x is displacement and F(t) is the external force
Homogeneous equation mx¨+cx˙+kx=0 represents free vibration without external forces
Particular solution represents the steady-state response to an external force
Laplace transforms used to solve differential equations by transforming them into algebraic equations
Transfer functions relate input (force) to output (displacement) in the Laplace domain
Fourier series represents periodic functions as a sum of sinusoidal components
Helps analyze the frequency content of vibration signals
Free Vibration Analysis
Undamped free vibration occurs when there is no damping (c=0) and no external force (F(t)=0)
Equation of motion simplifies to mx¨+kx=0
Solution is harmonic motion: x(t)=Acos(ωnt+ϕ), where A is amplitude and ϕ is phase angle
Natural frequency (ωn) for undamped systems: ωn=mk
Damped free vibration includes the effect of damping (c>0) without external forces
Equation of motion: mx¨+cx˙+kx=0
Damping ratio (ζ) characterizes the level of damping: ζ=2kmc
Underdamped (0<ζ<1): oscillatory motion with decreasing amplitude