Sdof vibration theory pdf

This chapter examines the free unforced vibration response and associated properties for various types of linear vibration system models. Theoretical study of the effects of nonlinear viscous damping. A free vibration is one that occurs naturally with no energy being added to the vibrating system. If however, any of the basic components behave nonlinearly, the vibration is called nonlinear vibration. The initial theory was applicable for an undamped sdof system subjected to a sinusoidal force excitation. Crandall department of mechamcal enghleerhtg, massachusetts institute of technology, cambridge, iassachusetts, u. Finally, we solve the most important vibration problems of all. Fundamentals of structural vibration school of civil and. The free vibration analysis of a system typically consists of determining natural frequencies, damping ratios, mode shapes, and the vibration due to imposing initial conditions ics on displacements and velocities. Force plate for corrugated container vibration tests. Force can be applied both as an external force ft, or as a base motion yt, as shown. An introduction to random vibration revision b by tom irvine email. The theory is then extended to mdof systems, where the tmd is used to dampen out the vibrations of a specific mode. The prototype for a lossless vibration system is the simple springmass model shown in figure 4a.

This example will be used to calculate the effects of vibration. The equations of motion for the forced vibration case also lead to frequency response of the system. The oscillations may be periodic such as the motion of a pendulum or random such as the movement of a tire on a gravel road. The function ut defines the displacement response of the system under the loading ft. Sdof harmonically forced vibration purdue university. Today, random vibration is thought of as the random motion of a structure excited by a random input. Logarithmic decrement from the damped vibration solution, the amount of damping in the system can be expressed as and the log decrement becomes and for small damping t n d t n d n 1 d n 1 lne e e. Derivation derive the dynamic governing equation of. Fema 451b topic 3 notes slide 2 instructional material complementing fema 451, design examples sdof dynamics 3 2 structural dynamics equations of motion for sdof structures structural frequency and period of vibration behavior under dynamic load dynamic magnification and resonance effect of damping on behavior linear elastic response spectra. Describes free vibration, the ode, natural frequency, and natural period. A sdof linear system subject to harmonic excitation with forcing frequency w. Forced vibration of singledegreeoffreedom sdof systems dynamic response of sdof systems subjected to external loading governing equation of motion m. Structural testing part 2, modal analysis and simulation br0507.

In engineering practice, we are almost invariably interested in predicting the response of a structure or mechanical system to external forcing. Structural testing part 2, modal analysis and simulation. Mar 03, 2015 this video is an introduction to undamped free vibration of single degree of freedom systems. Optimum configuration for vibration absorbers of a sdof. To obtain the time solution of any free sdof system damped or not, use the sdof calculator. Sdof, free vibration undamped and damped systems week 2. Instructional material complementing fema 451, design examples sdof dynamics 3 4 idealized sdof structure mass stiffness damping ft ut, t ft t ut the simple frame is idealized as a sdof massspringdashpot model with a timevarying applied load. Forced vibration of singledegreeoffreedom sdof systems. Part 3 covers the resposne of damped sdof systems to. When the exciting force is a steadystate sinusoid with frequency to there is a steadystate. Vibrations in free and forced single degree of freedom. Deflection calculation based on sdof method for axially.

The free vibration analysis of a system typically consists of determining natural frequencies, damping ratios, mode shapes, and the vibration due to imposing initial conditions ics on displacements and. In the frequency domain, analysis of the time signal gives us a spectrum containing a series of peaks, shown below as a set of sdof response spectra. Underdamped systems when characteristic equation has a pair of complex conjugate roots. Structural dynamics of linear elastic singledegreeof.

Random forcing function and response vibrationdata. Mod01 lec11 free and forced vibration of single degree of freedom systems. Numerical evaluation of dynamic responses, earthquake excitations week 4. The weighting, often called the modal participation factor, is a function of excitation and mode shape coeffi. A vibration is a fluctuating motion about an equilibrium state. May 22, 20 mod01 lec11 free and forced vibration of single degree of freedom systems. The natural free vibration is simple harmonic motion with frequency to n xkm. Notice that when the damping is 1 2, then there is the maximum response without having a peak in the response curve. Multiple degreeoffreedom systems are discussed, including the normalmode theory of linear elastic structures and lagranges equations. The differential equations that govern the behaviour of vibratory non.

Free vibration of a undercritically damped sdof system and thus oscillates about its equilibrium position with a progressively decreasing amplitude 2. Vibration refers to mechanical oscillations about an equilibrium point. Suppose that we need to stop a structure or component from vibrating e. The force plate can be used to determine the generalized sdof properties of an mdof system. If we examine a freebody diagram of the mass we see that the forces acting on it include gravity the weight and the resistance provided by the spring. Structural dynamics department of civil and environmental engineering duke university henri p. Abstractionmodeling idealize the actual structure to a simpli. This video is an introduction to undamped free vibration of single degree of freedom systems. If chapter 3 vibration isolation force transmitted notice that motion transmitted from the supporting structure to the mass m is less than one when the frequency ratio is greater that square root 2. Mod01 lec11 free and forced vibration of single degree.

Liu 12 used the fixedpoints theory and derived the optimum parameters. In vibration the system eigenvalues defines the natural frequencies, and the system eigenvectors defines the mode shapes. Free vibration of singledegreeoffreedom sdof systems procedure in solving structural dynamics problems 1. Viscous damping the most common form of damping is viscous damping. The mathematical theory of random vibration is essential to the realistic modeling of structural dynamic systems. Dynamics of simple oscillators single degree of freedom systems. Wong proposed an alternative design for proceedings of the imacxxvii february 912, 2009 orlando, florida usa 2009 society for experimental mechanics inc. Furthermore, the turbulent pressure at a particular location on the wing varies in a. Free vibration response vibration theory and applications. Unit 7 vibration of mechanical vibration of mechanical. Derivation derive the dynamic governing equation of the simpli. Gavin fall, 2018 this document describes free and forced dynamic responses of simple oscillators somtimes called single degree of freedom sdof systems. Free vibration of damped sdof system modeling of damping is perhaps one of the most dicult task in structural dynamics. Con tents preface xi chapter1 introduction 11 primary objective 1 12 elements of a vibratory system 2 examples of vibratory motions 5 14 simple harmonic motion 15 vectorial representation of harmonic motions 11 16 units 16 17 summary 19 problems 20 chapter 2 systems with one degree of freedomtheory 21 introduction 23 22 degrees of freedom 25 23 equation of motion.

The book begins by discussing free vibration of singledegreeoffreedom sdof systems, both damped and undamped, and forced vibration harmonic force of sdof systems. This chapter presents the theory of free and forced steadystate vibration of single degreeoffreedom systems. The coordinate xt is the absolute motion of the mass. Probability density function the histogram in figure 4 can be converted to a probability density function. The role of mechanical vibration analysis should be to use mathematical tools for. This article summarizes the work of some key contributors to the theory of random vibration from. Accelerated vibration testing based on fatigue damage. Introduction vibration is the motion of a particle or a body or system of connected bodies displaced from a position of equilibrium 1. This would be done by dividing each bar by the total number of samples, 4000 in this case. Based on numerical simulation and theoretical analysis, the impact response and deflection calculation method for axially loaded cfst members subjected to lateral impact are investigated in this paper. Pdf structural dynamics theory and applications download. Free vibration of a undercritically damped sdof system.

In practice, every object is subject to a certain level of vibration, which can often not be seen with the naked eye. It can be written as a weighted summation of sdof systems shown in figure 1. Free vibration no external force of a single degreeoffreedom system with viscous damping can be illustrated as, damping that produces a damping force proportional to the masss velocity is commonly referred to as viscous damping, and is denoted graphically by a dashpot. Like the harmonic sdof forced response example, the present example is also an example i let all my mechanical vibration students solve. The most basic vibration analysis is a system with a single degree of freedom sdof, such as the classical linear oscillator clo, as shown in fig. In each case, when the body is moved away from the rest position, there is a natural force that tries to return it to its rest position. Response to periodic dynamic loadings and impulse loads are also discussed, as are two degrees of freedom linear system response methods and free vibration of multiple degrees. Undamped systems and systems having viscous damping and structural damping are included. Undamped free vibrations consider the singledegreeoffreedom sdof system shown at the right that has only a spring supporting the mass. Intro to structural motion control purdue university. Reeeired 28 july 1969 in many applications of vibration and wave theory the magnitudes of the damping forces are small in comparison with the elastic and inertia forces. Structural dynamics of earthquake engineering sciencedirect. Furthermore, the mass is allowed to move in only one direction.

The solutions listed in the preceding sections give us general guidelines for engineering a system to avoid or create. Introduction to undamped free vibration of sdof 12. Axial force has a great influence on the dynamic behavior and the impact resistance of concretefilled steel tubular cfst members. Our primary objective in building the plate was to experimentally confirm the conclusions set forth by an earlier theory 2. Optimum configuration for vibration absorbers of a sdof system using genethic algorithm m. A deterministic vibration is one that can be characterized precisely, whereas a random vibration only can be analyzed statistically. A may be obtained by a function in the form x ert where r is a constant to be determined. Liu 12 used the fixedpoints theory and derived the optimum parameters of system leading to the minimum vibration amplitude at resonance. Here is the extension of the spring after suspension of the mass on the spring.

Principal modes 44 generalized and coupling 45 principal coordinates 158 46 modal analysis. The prototype single degree of freedom system is a springmassdamper system in which the spring has no damping or mass, the mass has no sti. This implies that the natural frequency of the supported system must be very small compared to the disturbing frequency. Generalized sdof systems, introduction to multi degree of freedom systems 88. The body is in equilibrium under the action of the two forces.

A common source of objectionable noise in buildings is the vibration of machines that are mounted on floors or walls. Obviously, the best place to mount a vibrating machine is on the ground floor. Dynamics of simple oscillators single degree of freedom. The concept of the output frequency response function ofrf recently proposed by the authors is applied to study how the transmissibility of a sdof vibration isolator. Pdf prediction of seismic energy dissipation in sdof systems. It is still a topic of research in advanced structural dynamics and is derived mostly experimentally. Jan 15, 2016 this chapter examines the free unforced vibration response and associated properties for various types of linear vibration system models. In the time domain the vibration or acoustic response of the bell is shown as a time history, which can be represent ed by a set of a decaying sinusoids. Forced vibrations harmonic, periodic, arbitrary excitations week 3.

The nonlinear numerical model of an axially loaded cfst. The supplied zip file contains a pdf file with the problem definition, and a separate zip file with a suggested solution. Most manufacturers of seismometers attempt to achieve this level of damping. Some single degree of fdfreedom sdof systems with an external force are shown in the figure. Mod01 lec11 free and forced vibration of single degree of. Dynamics of simple oscillators single degree of freedom systems cee 541. This example will be used to calculate the effects of vibration under free and forced vibration, with and without damping. Our primary objective in building the plate was to experimentally confirm the conclusions set forth by an earlier theory. The words incidentally are derived from the german word eigen, meaning own, so the eigenvalues of a set of equations are its own values, and the eigenvectors are its own vectors. Theory and applications has been adapted to incorporate the.

113 171 1357 1231 1027 1287 992 827 272 1535 102 249 1382 318 691 882 368 695 490 303 1561 1001 540 588 1130 1110 830 332 337 269 1126 441 1081 858 338