theory of vibration with applications thomson ch1 kuliah

8/12/2019 Theory of Vibration With Applications Thomson Ch1 Kuliah

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scillatory otionThe study of vibration s concerned with the oscillatory motions of bodies and theforces associated with them. All bodies possessing mass and elasticity are capable ofvibration.1l1us. most engineering machines and structures experience vibration to somedegree, and their design generally requires consideration of their oscillatory behavior.Oscillatory systems can be broad ly characterized as linear or nonlinear. For linearsystems. the principle of superposition holds, and the mathematical techniques available for their treatment are well developed. In contrast, techniques for the analysis ofnonlinear systems are less well known and difficult to apply. However, some knowledge of nonlinear systems s desirable, because all systems tend to become nonlinearwith increasing amplitude of oscillation.

There are two general classes of vibrations-free and forced. Free vibration takesplace when a system oscillates under the action of forces inherent n the system itself,and when external impressed forces are absent. The system under free vibration willvibrate at one or more of its natural frequencies , which are properties of the dynamicalsystem established by its mass and stiffness distribution.

Vibration that takes place under the excitation of external forces s called forcedvibration. When the excitation s oscillatory, the system s forced to vibrate at the excitation frequency. I f the frequency of excitation coincides with one of the natural frequencies of the system , a condition of resonance s encountered and dangerously largeoscillations may result.ll1e failure of major structures such as bridges, buildings, or airplane wings s an awesome possibility under resonance. Thus, the calculation of thenatural frequencies s of major importance in the study of vibrations.

Vibrating systems are all subject to damping to some degree because energy sdissipated by friction and other resistances. f the damping s small, it has very littleinfluence on the natural frequencies of the system, and hence the calculations for thenatural frequencies are generally made on the basis of no damping. On the other hand ,damping s of great importance in limiting the amplitude of oscillation at resonance.

The number of independent coordinates required to describe the motion of a system s called degrees o reedom of the system. Thus, a free particle undergoing generalmotion n space will have three degrees of freedom , and a rigid body will have six

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6 Chapter 1 Oscillatory Motion

FIGURE 1.1.1 . Recording harmonic motion.degrees of freedom , i.e., three components of position and three angles defining its orientation. Furthermore, a continuous elastic body will require an infinite number ofcoordinates three for each point on the body) to describe its motion ; hence, itsdegrees of freedom must be infinite. However, in many cases, parts of such bodies maybe assumed to be rigid, and the system may be considered to be dynamically equivalent to one having finite degrees of freedom . In fact, a surprisingly large number ofvibration problems can be treated with sufficient accuracy by reducing the system toone having a few degrees of freedom .

1 1 H RMONIC MOTION

Oscillatory motion may repeat itself regularly, as in the balance wheel of a watch, ordisplay considerable irregularity, as in earthquakes. When the motion is repeated inequal intervals of time T it is called periodic motion. 1l1e repetition time Tis called theperiod of the oscillation, and its reciprocal, f = 1/T is called the frequency. f themotion is designated by the time function x t), then any periodic motion must satisfythe relationship x t) = x t T .

The simplest form of periodic motion is harmonic motion. t can be demon-strated y a mass suspended from a light spring, as shown in Fig. 1.1.1. f the mass isdisplaced from its rest position and released , it will oscillate up and down . By placing alight source on the oscillating mass, its motion can be recorded on a light-sensitive filmstrip, which is made to move past it at a constant speed.

The motion recorded on the filmstrip can be expressed by the equation

X_ . . . . - -

. tx A stn Ti-T

I--- -- -_ __::_:: -___ .- FIGURE 1.1.2. Harmonic motion as a projection of a point moving on a circle.

w

1.1.1)


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Section 1.1 Harmonic Motion 7where A is the amplitude of oscillation measured from the equilibrium position of themass, and Tis the period .The motion is repeated when t = T

Harmonic motion is often represented as the projection on a straight line of apoint that is moving on a circle at constant speed , as shown in Fig. 1.1.2. With the an gular speed of the line 0 p designated by w the displacement x can be written as

x = A sin wt (1.1.2)The quantity w is generally measured in radians per second and is referred to as

the circular frequency. 1 Because the motion repeats itself in 21r radians, we have therel ationship

7TV = - = 27TfT ( 1.1.3)

where T and fare the period and frequency of the harmonic motion , usually measuredin seconds an d cycles per second, respectively.

1l1e velocity and acceleration of harmonic motion can be simply determined bydifferentiation of Eq. (1.1.2). Using the dot notation for the der ivative, we obtainx= wA cos wr = wA sin wl + 7r/2)

x = - w- A sin wl = w- A sin wl + r ? ) ( )(1.1.4)(1.1.5)

Thus, the velocity and acceleration are also harmonic with the same frequency of oscillation , but lea d the displacement by 7r, 2 and r radians, respectively. Figure 1.1.3 showsboth time variation and the vector phase relationship between the displacement , velocity, and acceleration in harmonic motion .

Examination of Eqs. (1. 1.2) and (1.1.5) reveals that ?x = w -x

a) b)FIGURE 1.1.3. In harmoni c motion. the ve locity and acceleration lead the displaceme nt byrr/ 2 and 7T.

(1.1.6)

The word circular is genera lly del e led. and cv and fare used without distinction for frequ ency.


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8 hapter 1 Oscillatory Motionso that in harmonic motion , the acceleration is proportional to the displacement and isdirected toward th e origin. Because Newton s second law of motion states that theacceleration is proportional to the force , harmonic motion can be expected for systemswith linear springs with force varying as kx .

Exponential form The trigonometric fun ct ions of sine and cosine are related tothe exponential function by Euler s equation

ei = cos e+ i sin e (1.1.7)A vector of amplitude A rotating at constant angular speed w can be rep resented as acomplex quantity z in the Argand diagram, as shown in Fig. 1.1.4.

= A cos wt + iA sin wt (1.1.8)= X + iy

The quantity z is referred to as the omplex sinusoid, with x andy as the rea l and imag-in ary components, respec ti vely. The quantity z = eiw also satisfies th e differentialequation L1.6) fo r harmonic motion .

Figure 1 1 5 shows z and its conjugate z* = e - iwr which is rotating in the nega-tive direction with angula r speed - w. It is evident from this diagram that th e real com ponent xis expressible in terms of z and z* by the equation

x =Hz+ z* A cos wt = ReAe ;' 1 (1.1.9)where Re stands for the real part of the quantity z We will find that the exponentialform of the harmonic motion often offers mathematical advantages over the trigono-metric form.

Some of the rules of exponential operations between z 1 = A 1e;e, and z 2 = A 2 e;e,are as follows :Multipl ication zl z AI A2 e; e,+e)Division e; (e,-e,) (1.1.1 0)

y y

X

FIGURE 1.1.4 . Harm o nic motionrepresen ted by a rotating vector.

FIGURE 1.1.5 . Vector z and its co njuga te z .

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Section 1.2 Periodic Motion 9Powers

1 2 PERIODIC MOT ONt is quite common for vibrations of several different frequencies to exist simultane-

ously. For example , the vibration of a violin string is composed of the fundamental frequency .f and all its harmonics, 2 j ~ 3{, and so forth. Another example is th e freevibration of a multidegree of freedom system, to which the vibrations at each naturalfrequency contribute. Such vibrations result in a complex waveform , which is repeatedperiodically as shown in Fig. 1.2.1.

ll1e French mathematician J. Fourier ( 1768 - 1830) showed that any periodicmotion can be represented by a series of sines and cosines that are harmonically re la ted.If x t) is a periodic function of the period T, it is represented by the Fourier seri es

( ) aox I = - + a 1 cos w 1t + a? cos , l + 2 - - ( 1.2.1)where

T

To determine the coefficients a

and b

, we multiply both sides of Eq. ( 1.2.1) by cos w,t orsin w t and integrate each te rm over th e period T. By recognizing the following relations,

x t

i fm -= = nJ- j ?, - cos w,t cos w,,/ dt = { 01,12 T 2 if m = n

Jr 2

sin w,,t sin w11,t dt = { 01r/ 2 T 2

if m-= = ni fm = n

- T - ..FIGURE 1.2 . Periodic motion of period r

( 1.2.2)


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1 Chapter 1 Oscillatory otionT/ 2I COS W / sin W 111f eft = {-r l2 0 i m I nif m = n

all terms except one on the right side of the equation will be zero, and we obtain theresult

an2 J / 2- x(t) cos wilt dtT - T/2

bll = I / l x(t) sin wilt dtT - T/2

(1.2.3)The Fourier series can also be represented in terms of the exponential function.

Substituting

in Eq. (1.2.1) , we obtainx(t) = Go + :L [ (a - ib )eiw,,l + (a + ib )e - iw, ]n = l :? n n n n

(1.2.4)

n = :.c

whereICo = ao

ell = - ibJ (1.2.5)Substituting for a

and b from Eq . 1 .2.3), we find c, to be

I J ;C

= - x(t) cos w,J - i sin w,J dt

T - /2T/2~ I x(t)e-iw,l dt

T - /2(1.2.6)

Some computational effort can be minimized when the function x(t) is recogniz-able in terms of the even and odd functions:

x(t) = E(t) + O(t) (1.2.7)An even function E(t) is symmetric about the or igin , so that E(t) = E( -t , I.e.,cos wt = cos (-wr . An odd function satisfies the relationship O(t) = - 0 -t , I.e.,sin wt = - sin - wt). The following integrals are then helpful:


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Section 1 3 Vibration Terminology

0.40.3 ..._ _ ..._ '0.2 .... '0.1

0 0 2 3 4 5 6 7 8 9 10 II 12 n

/ // /

n

FIGURE 1.2.2. Fourier spectrum for pulses shown in Prob. 1.16. k =

I /2

E t) sin w / t = 0/ 2I / 2- T 2O t) cos W,/ t = 0

(1.2.8)

When the coefficients of the Fourier series are plotted against frequency w

theresult is a series of discrete lines called the Fourier spectrum. Generally plotted are theabsolute va lues l2cnl = v a;, + and the phase = tan - 1(bja,), an example ofwhich is shown in Fig. 1.2.2. Fourier analysis including the Fourier transform are discussed in more detail in Chapter 13.

With the aid of the digital computer, harmonic analysis today is efficiently carried out. A computer algorithm known as the fast Fourier tran4orm 2 (FFT) is commonly used to minimize the computation time.

1.3 VIBR TION TERMINOLOGYCertain terminologies used in vibration analysis need to be represented here. The simplest of these me the peak value and the average value.

The peak value generally indicates the maximum stress that the vibrating part isundergoing. It also places a limita tion on the rattle space requirement.

The average value indicates a steady or sta tic value, somewhat like the de level ofan electrical current. It can be fou nd by the time integral

Tx = lim _ J t) dt (1.3.1)T--> x T ll

2See J. S. Benda and A . G Piersol. Random Dma (New York: Joh n Wiley. 1971 ). pp. 305-306.l


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12 Chapter 1 Osci llatory MotionFor example, the average value for a complete cycle of a sine wave, A sin t , is zero;whereas its average value for a half-cycle is

x = f sin t dt = 2A = 0.637A7T ) 7T

t is evident that this is also the average value of the rectified sine wave shown in Fig. 13 1The square of the displacement gene rally is associated with the energy of the

vibration for which the mean square value is a measure. The mean square value of atim e function x t) is found from the average of the squared va lues, integrated over sometime interval T: - ] Tx 2 = lim T x 2t d7 > N 0For example, if x t) = A sin wr, its mean square value is

- A2J 1x 2 lim 1 cos2wt)dt =T n T 0 2

1 7- k2

(1.3.2)

The root mean square rms) value is the square root of the mean square value.From th e prev ious ex ample, the rms of the sine wave of amplitude A isA/V2 = 0.707A. Vibrations are commonly measured by rms meters.

The decibel is a unit of measurement that is frequently used in vibration mea-surements. It is defined in terms of a power ratio.dB = 10 log10(

(1.3.3)= 10 log O( r

The second equation results from the fact that power is proportional to the square ofthe amplitude or voltage. Th e decibel is often expressed in terms of the first power ofamplitude or voltage as

dB = 20 log X )x2Thus an amplifier with a voltage gai n of 5 has a decibel gain of

20 log 10(5) = + l4

FIGURE 1.3.1. Averagevalue of a rect ified sine wave.

x f)

(1.3.4)


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Problems 13Because the decibel is a logarithmic unit, it compresses or expands the scale.

When the upper limit of a frequency range is twice its lower limit, the frequencyspan is said to be an octave For example, each of the frequency bands in the followingtable represents an octave band

Band Frequency Range Hz) Frequency BandwidthI 10-20 lO2 20-40 203 40-80 404 200-400 200

PRO LEMSl L A ha rmonic motion has an amplitude of 0.20 em and a period of 0.15 s Determine the

maximum velocity and acceleration.1 2 An accelerometer indicates that a structure is vibrating harmonically at 82 cps with a

maximum acceleration of 50 g Determine the amplitude of vibration.1 3 A harmonic motion ha s a frequency of 10 cps and its maximum velocity is 4.57 m / s

Determine its amplitude. its period , and its maximum acceleration.1 4 Find the sum of two harmonic motions of equal amplitude but of slightly different fre-

quencies. Discuss the beating phenomena that result from this sum.1 5 Express the complex vector 4 3i in the exponential form e 81 6 Add two complex vectors (2 3i) and (4 - i) , expressing the result as A L 6.1 7 Show that the multiplication of a vector z = A e;, , by i rotates it by 90.1 8 Determine the sum of two vectors 5ei"/6 and 4ei IJ and find the angle between the resul

tant and the first vector.1 9 Determine the Fourier series for the rectangular wave shown in Fig. Pl.9.

FIGURE P1.9.

1 10 If the o rigin of the square wave of Prob. 1.9 is shifted to the right by 7T/ 2. determine theFourier series.

1 11 Determine the Fourier series for the triangular wave shown in Fig. Pl.ll.

w 1 tFIGURE P1.11 .


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4 Chapter 1 Oscillatory Motion1 12 Determine the Fourier series for the sawtooth curve shown in Fig. Pl.l2. Express the

result of Prob. 1.1 2 in the exponential form of Eq. (1.2.4).

x t)

FIGURE P1.12.

1 13 Determine the rms value of a wave consisting of the positive portions of a sine wave.1 14 Determine the mea n square va lu e of the sawtooth wave of Prob. J 12. Do this two ways.

from th e squared curve and from the Fourier series.L 15 Plot the frequency spectrum for the triangular wave of Prob. J.ll.1 16 Determine the Fourier s e r ~ e s of a series of rectangular pulses shown in Fig. P 1.16. Plot c

and versus n when = .

..-- 1.0

1 2rr j ~ j k r r ~FIGURE .16.

1 17 Write the equ a tion for the displacements of the piston in the crank-piston mechanismshown in Fig. P1.17. and determin e the harmonic components and their re lative magni-tudes. If r I = Lwhat is the ratio of the second harmonic compared to the first?

FIGURE P1.17 .1 18 Determine the mea n square of the rectangular pulse shown in Fig. PI 18 fork = 0.10. If

the ampiitude is A what would an rms voltmeter read?

T J Im mIGURE P1.18.

1 19 Determine the mea n square value of the triangular wave of Fig. Pl.l l .1 20 An rms voltmeter specifies an accuracy of : ::0.5 dB. If a vibration of 2.5 mm rms is mea

sured. dete rmine the millimeter accuracy as rea d by the voltmeter.


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Problems 51 2l Amplification factors on a voltmeter used to measure the vibration output from an

acceleromete r are given as 10 , 50 , and I 00. What are the decibel steps?1 22 TI1c calibration curve of a piezoelectric acce lerometer is shown in Fig. Pl.22 where the

ordinate is in decibels. If the peak is 32 dB, what is the ratio of the resonance response tothat at some low frequency, say. 1000 cps?

( )0EQ .E0CllD

3 0 t - 20 - 10 _::_ - - :::: ::: / -- l

f - - - -- - _ v . l0 \

r --- l-1 0 - - -- - - \-2 0 1- - - - -- - ~

100 1000 10000 100000FIGURE P1.22.

1 23 Using coordinate paper similar to that of Appendix A. outline the bounds for the following vibration specifications. Max. acceleration = 2 g. max . displacement = 0.08 in. , min.and max. frequencies: I Hz and 200Hz.

1 24 Assume a pulse occurs at int eger times and lasts for I second. It has a random ampl itudewith th e probability of having the amplitude equal 1 or -1 being p 1 = p( - l = 1/ 2.What is the mean value and the mean square value of the amplitude'/

1 25 Show that every function j t) can be represented as a sum of an odd function O t) and aneven function E t).

theory of vibration with applications thomson ch1 kuliah

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