Vibration Reduction and Stability of Non-Linear. System Subjected to External and Parametric. Excitation Forces under a Non-Linear Absorber
|
|
- Cornelius Francis
- 5 years ago
- Views:
Transcription
1 Int. J. Contemp. Math. Sciences, Vol.,, no., 5-7 Vibration Reduction and Stability of Non-Linear System Subjected to Eternal and Parametric Ecitation Forces under a Non-Linear Absorber M. Sayed *, Y. S. Hamed * and Y. A. Amer ** Department of Mathematics and Statistics, Faculty of Science, Taif University El-Taif, El-Haweiah, P.O. Bo, Zip Code 97, Kingdom of Saudi Arabia eng_yaser_salah@yahoo.com * Faculty of Electronic Engineering, Menoufia University, Menouf 95, Egypt ** Department of Mathematics, Faculty of Science, Zagazig University Zagazig, Egypt Abstract Vibrations are usually undesired phenomena as they may cause discomfort, disturbance, damage, and sometimes destruction of machines and structures. It must be reduced or controlled or eliminated. One of the most common methods of vibration control is the dynamic absorber. In this paper, the non-linear dynamics of a two-degree-of freedom vibration system including quadratic and cubic non-linearities subjected to eternal and parametric ecitation forces is investigated. The system consists of the main system and the absorber which represents many applications in machine tools, ultrasonic cutting process, etc. The vibration of the main system can be controlled applying non-linear absorber (passive control). The stability of the system is investigated using both frequency response curves and phase-plane trajectories. Multiple time scales perturbation method is applied to differential equations describing the system to obtain the analytical solution. All possible resonance cases are etracted. The effects of different parameters of the system are studied numerically. There eist multi-valued solutions which increase or decrease by the variation of some parameters. The solution loses stability on increasing negative value of α. The Numerical simulations show the system ehibits periodic motions and chaotic motions. A comparison is made with the available published work.
2 5 M. Sayed, Y. S. Hamed and Y. A. Amer Keywords: Non-linear vibration; response; stability; resonance; jump phenomenon. Introduction The dynamic response of mechanical and civil structures subject to highamplitude vibration is often dangerous and undesirable. Sometimes controlled vibration is desirable as in ultrasonic machining (USM), as the machining technique is dependent on tool and abrasive particles vibration. It is required to reduce the vibration in the machine head and have reasonable amplitude for the tools. This can be done via dynamic absorber. It has the advantages of low cost and simple operation at one modal frequency. In the domain of many mechanical vibration systems the coupled non-linear vibration of such systems can be reduced to non-linear second order differential equations which are solved analytically and numerically. Queini and Nayfeh [] proposed a non-linear active control law to suppress the vibrations of the first mode of a cantilever beam when subjected to a principal parametric ecitation. The method of multiple scales is applied throughout. The analysis revealed that cubic velocity feedback reduced the amplitude of the response. Asfar [] took material non-linearity into consideration in the analysis of the performance of an elastomeric damper with a spring hardening cubic effects near primary resonance condition applying multiple time scale method. Eissa [] reported that when using a dynamic absorber, its damping coefficient should be kept minimal for better system performance. Eissa [] has shown that for controlling the vibration of a system subjected to harmonic ecitations, the fundamental or the first harmonic absorber is the most effective one. Eissa and El-Ganaini [5, ] studied the control of both vibration and dynamics chaos of mechanical system having quadratic and cubic non-linearities, subjected to harmonic ecitation using multi-absorbers. Kamel and Amer [7] studied the behavior of one-degree-of-freedom system with different quadratic damping and cubic stiffness non-linearities simulating the aial vibration of a cantilever beam under multi-parametric ecitation forces. Song et al. [] investigated the vibration response of the spring mass damper system with a parametrically ecited pendulum hinged to the mass using the harmonic balance method. The stability analysis showed that the area of unstable motion of the system obtained from the third order approimation. Soom [9] and Jordanov [] studied the optimal parameter design of linear and non-linear dynamic vibration absorbers for damped primary systems. They eamined optimization criteria other than the traditional one and obtained small improvements in steady state response by using non-linear springs. However, the presence of the non-linearities introduces dangerous instability, which in some cases may result in amplification rather than reduction of the vibration amplitudes [, ]. Natsiavas [] applied the method of averaging to investigate the steady state oscillations and stability of non-linear dynamic vibration absorbers. He pointed out that proper selection of the system parameters would result
3 Vibration reduction and stability of non-linear system 5 insubstantial improvements of non-linear absorbers and avoid dangerous effects that are likely to occur due to the presence of the non-linearities. Zhu et al. [] studied the non-linear dynamics of a two-degree-of freedom vibrating system having both non-linear damping and non-linear spring using the averaging method. Results showed that the vibration amplitude can be reduced by properly selecting the values of non-linear damper, non-linear spring stiffness and the range of eciting frequency. Lim et al. [5] investigated the behavior of the (USM) hypothesized theoretical model which described by the coupling of two non-linear oscillators. The method of multiple scales has been used to solve the equations to first order perturbation. The theoretical results showed that controlled variations in the softening stiffness can have a significant effect on the overall non-linear response of the system, by making the overall effect hardening, softening, or approimately linear. Eperimentally, it has also been demonstrated that coupling of ultrasonic components with different non-linear characteristics can strongly influence the performance of the system. Eissa and Amer [] simulated the vibration of a second order system to the first mode of a cantilever beam subjected to both eternal and parametric ecitation at primary and sub-harmonic resonance. They analyzed the system using the method of multiple scales. They reported that the vibration of the system can be controlled by adding a feedback cubic non-linear term. They reported also that there is a threshold value for the linear damping coefficient which can be applied to control the system vibration. Nayfeh [7] compared application of the method of multiple scales with reconstitution and the generalized method of averaging for determining higher-order approimations of three single-degree-of-freedom systems and a two-degree-of-freedom system. He showed that the second-order frequency-response equation possesses spurious solutions for the case of softening nonlinearity. El-Bassiouny [] investigated the effects of quadratic and cubic non-linearities in elastomeric material dampers on torsional vibration control. The multiple time scale is used to solve the stability equations at primary resonance. He showed that the elastomeric damper reduced the vibration of the crankshaft effectively. Eissa et al. [9, ] presented the tuned absorber in both transversely and longitudinal directions of a simple pendulum which designed to control one frequency at primary resonance. The multiple time scale perturbation technique is applied throughout. They demonstrated the effectiveness of the absorber for passive control. They reported that the vibration of the system can be controlled actively via negative velocity feedback, which can be used to reduce the amplitude of the system. Amer [] investigated the coupling of two non-linear oscillators of main system and absorber representing ultrasonic cutting process subjected to parametric ecitation forces. A threshold value of main system linear damping has been obtained, where vibration can be reduced dramatically. This threshold value can be used effectively for passive vibration control, if it is economical. The multiple time scale perturbation technique is applied throughout. A threshold value of linear damping has been obtained, where the system vibration can be reduced dramatically.
4 5 M. Sayed, Y. S. Hamed and Y. A. Amer Hamed et al. [-5] studied USM model subject to multi-eternal or both multi-eternal and multi-parametric and both multi-eternal and tuned ecitation forces. The model consists of multi-degree-of-freedom system consisting of the tool holder and absorbers (tools) simulating ultrasonic machining process. The advantages of using multi-tools are to machine different materials and different shapes at the same time. This leads to time saving and higher machining efficiency.. Passive Control Using a non-linear tuned mass absorber connected to the main system, a model of a two degree-of-freedom oscillator under consideration is shown in Fig., from the principles of the mechanics, the derived equations of motion can be written in the forms: && +ω +εα +εα +εζ & +εζ & +εζ( & & ) εα +εα ( ) + εα ( ) = εf cosω t + ε F cosω t () 5 && + ω ( ) + εβ ( ) + εβ ( ) + εζ ( & & ) = () m k F cos Ωt + F cos Ω t m c k c Fig.. Schematic diagram of the model with absorber. where k ω = + k k, α = k, α = c, ζ = c, ζ = c, ζ = k, α =,, m m m m m m m k k f j k c k k α =, α 5 =, Fj =, ω =, ζ =, β =, β = m m m m m m m c, c are the damping coefficients of the main system and absorber, c the coupling damping coefficient, m, m the mass of the main system and absorber,
5 Vibration reduction and stability of non-linear system 55 Ω j ( j=, ) forcing frequencies, ω, ω natural frequencies, k, k linear stiffness,, displacement of the main system and absorber, & j, && j derivatives of w. r. t time, ε small perturbation parameter, f j the forcing amplitudes, α i, β j non-linear parameters (i =,,5), ζs damping coefficient (s =,, ).. Method of Analysis A first-order uniform solution of equations ()-() is sought using the method of multiple scales [] in the form: ( t; ε ) = ( T, T) +ε ( T, T) +... () ( t; ε ) = ( T, T) +ε ( T, T) +... () where T o = t is fast time scale, which is associated with changes occurring at the frequencies ω j and Ω j and T = ε t is the slow time scale, which is associated with modulations in the amplitudes and phases resulting from the non-linearities and parametric resonance. In term of T o and T the time derivatives became d D D... dt = +ε +, d = D + ε DD+... (5) dt Where D n differential operators; Dn = / Tn ( n=,). Substituting equations () and () into equations ()-() and equating the coefficients of same power of ε in both sides, we obtain: Order ε : ( D +ω ) = () ( D +ω ) =ω (7) Order ε : ( D +ω ) = F cos( Ω T ) + F cos( ΩT ) D D α α ζd ζ( D ) ζ( D D ) +α α ( + ) α5( + ) () ( D +ω ) = D D +ω β( + ) β ( + ) ζ( D D ) (9) The general solution of equations ()-(7) can be epressed in the form iωt = Ae + cc () iωt iωt = Ae + A ω ( ω ω ) e + cc () where A and A are unknown functions in T, which can be determined from eliminating the secular terms at the net approimation, and cc stands for the conjugate of the preceding terms. The particular solutions of equations ()-(9) after eliminating the secular terms are given by:
6 5 M. Sayed, Y. S. Hamed and Y. A. Amer = Ue + Ue + Ue + He + He iωt i ( Ω +ω ) T i ( Ω ω ) T iωt iωt + H e + H e + H e + H e + H e i ω T iω T iω T i ( ω +ω ) T i ( ω ω ) T 5 7 i ( ω+ω ) T i ( ω ω ) T i ( ω+ ω) T i ( ω ω) T + H e + H9e + He + He + H + cc () iωt i( Ω +ω) T i( Ω ω) T iωt iωt = U e + U e + U e + H e + H e 5 + H e + H e + H e + H e + H e iω T iω T iω T i( ω +ω ) T i( ω ω ) T H e + H e + H e i( ω + ω ) T i( ω ω ) T i( ω + ω ) T i( ω ω) T H e H cc () where U i, i = to, H i, i = to, are comple functions in T. The general solution of and up to the first-order approimation is given by = +ε +..., = +ε Resonance Cases From the equations () to () all possible resonance cases are: (a) Trivial resonance: Ωj ω j =, j =,. (b) Internal resonance: ω nω, ω nω, n =,, (c) Primary resonance: Ω ω, Ω ω (d) Sub-harmonic resonance: Ω ω (e) Combined resonance: Ω ±ω ±ω (f) Simultaneous resonance: Any combination of the above resonance cases is considered as simultaneous resonance.. Stability Analysis The stability of the system is investigated at one of the worst resonance cases (confirmed numerically), which is the simultaneous primary, principal parametric and internal resonance where Ω ω, Ω ω and ω ω. Using the detuning parameters σ, σ and σ such that: Ω =ω +εσ, Ω = ω +εσ and ω = ω +εσ () Substituting equation () into equations ()-(9) and eliminating the secular terms leads to the solvability conditions as iω DA = [ iωζ +α iωζ ( ) ] A iωζ + α + α5( ) AA F i T A F i T i T α5( ) AAA + e σ + e σ + α5( ) A Ae σ (5) i σt i ω D A = i ω ζ A + ω + β ( ) A e + ω A β A A β ( ) AAA () where =ω ( ω ω ), = i ωζ +α +α5( ) ω
7 Vibration reduction and stability of non-linear system 57 and = i ωζ + α + α5aa( ) + α 5A A ( ω ω ) We epress the comple function A n in the polar form as i n ( T ) A n = ( ) a n ( T ) e μ ( n =,) (7) where a n and μ n are real. Substituting equation (7) into equations (5) and () and separating real and imaginary part yields, F F ζ +ζ( ) α5( ) ζ a = sin γ + sin γ a+ sin γ aa a () ω ω ω F F α α5( ) α5( ) μ a= cos γ cos γ + a+ aa cos γ aa ω ω ω ω ω α +α5( ) + a (9) ω a ζ + ζ ωζ = sin γ cos γ a ω a () α ( α+β 5 )( ) ( α+β 5 ) ωζ μ a = + + cos γ + sin γ ω a ω a a ω a ω a () ω( α +α5( ) ) β( ) where = + ω ω and γ = σt μ, γ = σt μ, γ = σt μ + μ () For the steady state solution a n = γ n =. Then from equation () yields μ =σ =σ /=σ, μ = σ σ () Then it follows from equations ()-() that the steady state solutions are given by F F ζ+ζ ( ) α5( ) ζ sin γ+ sin γ a+ sin γ aa a = () ω ω ω F F α α5( ) α5( ) aσ+ cos γ + cos γ + a aa + cos γ a a ω ω ω ω ω [α + α ( ) ]/ ω a = (5) { } 5 [ ] a [ ] a ( ζ +ζ ) / sin γ ( ω ζ / ω )cos γ = () α ( α+β 5 )( ) ( α+β 5 ) ( σ σ) ω ω ω a a a a a +cos γ +ωζ ( ω )sin γ a = (7) [ ] Solving the resulting algebraic equations yields two possibilities for the fied points for each case.
8 5 M. Sayed, Y. S. Hamed and Y. A. Amer Case (): The controller is deactivated ( a, a = ), the frequency response equation can be obtained in the form 9α σα ζ F F FF a a + σ + a a a cos( γ γ ) = () ω ω ω ω ω Case (): the controller is activated ( a, a ), the resulting two equations are obtained F F a + 5a + a + 7aa + aa + 9aa +aa a ω ω ( FF / ω ) a cos( γ γ ) = (9) a + a + a + a a + a a + a a + a = () 5 7 where ( i =,...,7) are given in the appendi. i. Numerical Results and Discussion To study the behavior of the main system, the Runge-Kutta fourth-order method was applied to the equation () governing the oscillating system, after eliminating all parameters corresponding to controller. Fig. shows the steady state amplitude and phase plane of the main system at the primary resonance where Ω ω for the parameters ζ =.5, F=., F =., α =., α =.. In this Figure, we observe that the steady state amplitude is about five of the ecitation force amplitude F. The main system is stable. d dt Time Fig.. System behavior without absorber at primary resonance Ω ω and Ω is a way from ω.
9 Vibration reduction and stability of non-linear system 59 Figs. and show the steady state amplitude and phase plane of the main system at the principle parametric and simultaneous primary and principle parametric resonance respectively where Ω ω and Ω ω, Ω ω. In these Figures, we note that the steady state amplitude is about 9 and of the ecitation force amplitude F respectively. Also the chaotic wave motion will increase. d dt Time Fig.. System behavior without absorber at principle parametric resonance Ω ω and Ω is a way from ω. Fig. 5 shows that the steady state amplitude of the system with absorber at the simultaneous primary and internal resonance Ω ω, ω ω. The effectiveness of the absorber E a ( E a = steady state amplitude of the system without absorber / steady state amplitude of the system with absorber) is about 5, which means that the steady state amplitude is reduced to less than % of the maimum amplitude shown in Fig.. d dt Time Fig.. System behavior without absorber at simultaneous resonance Ω ω and Ω ω. Also, the oscillations of the system and absorber have multi-limit cycle and chaotic, respectively. All solutions of the system and absorber are stable. Fig. shows that the steady state amplitude of the system with absorber at the simultaneous principal parametric and internal resonance Ω ω, ω ω. The effectiveness of the absorber Ea is about, which means that the steady state amplitude is reduced to less than % of the maimum amplitude shown in Fig.. Also, the oscillations of the system and absorber have multi-limit cycle and increasing dynamic chaos, respectively.
10 M. Sayed, Y. S. Hamed and Y. A. Amer d dt Time d dt Time Fig.5. Response of the system and absorber at simultaneous resonance Ω ω and ω ω. Fig. 7 shows that the steady state amplitude of the system with absorber at the simultaneous resonance Ω ω, Ω ω and ω ω. The effectiveness of the absorber Ea is about 7, which means that the steady state amplitude is reduced to less than % of the maimum amplitude shown in Fig.. Also, the oscillations of the system and absorber have multi-limit cycle and increasing dynamic chaos, respectively. d dt Time d dt Time Fig.. Response of the system and absorber at simultaneous resonance Ω ω and ω ω.
11 Vibration reduction and stability of non-linear system d dt Time d dt Time Fig.7. Response of the system and absorber at simultaneous resonance Ω ω, Ω ω and ω ω.. Theoretical frequency and force-response curves Case : The controller is deactivated, a, a = : The analytical analysis is represented graphically by using the numerical methods. The frequency response equation () is a nonlinear algebraic equation, which are solved numerically by using Newton Raphson method. The numerical results are shown in Figures -7. In all Figures, the region of stability of nontrivial solutions is determined by applying the Routh-Hurwitz criterion. The stable and unstable solutions are represented by solid and dotted lines respectively on the response curves. Figs -7 show the frequency-response and force-response curves for the stability first case. In Figs. -, we observe that the solutions is stable for negative values of σ and it has stable and unstable for positive values of σ. Fig. shows the effects of he detuning parameter σ on the steady state amplitude of the system. In this Figure, the response amplitude consists of a continuous curve which is bent to the right and has hardening phenomena. This continuous curve has stable and unstable solutions.
12 M. Sayed, Y. S. Hamed and Y. A. Amer a σ a α = α =. α =. - - σ Fig.. Effects of the detuning parameter σ Fig. 9. Effects of the nonlinear spring stiffness α a - - σ F = F = F = Fig.. Effects of the ecitation amplitude F a σ ω =. ω = ω =.5 Fig.. Effects of the natural frequencies Fig. 9 shows that as non-linear spring stiffness α is increased positively the continuous curve is moved downwards and has decreased magnitudes. It can be concluded that increasing the non-linear spring stiffness α can reduce the amplitude of the system and obtain the effect of reduction of the vibration amplitude. The regions of multi-valued and instability zone are increased and decreased respectively. Also for negative value of non-linear spring stiffness α the response amplitude is bent to the left and the stability region is decreased. The positive and negative values of the non-linear spring stiffness α produce either hard or soft spring, respectively. The steady state amplitude a is a monotonic increasing function in the ecitation amplitude F and for small values of F the single-valued curve is shifted upwards with decreased instability zone, as shown in Fig.. The zones of multi-valued and instability region are increased for large values of F. It is clear that from Fig. for decreasing natural frequency ω the steady state amplitude is increasing and the curve is bent to the right, leading to multi-valued amplitudes and to appearance of the jump phenomenon. From Fig., the steady state amplitude is a monotonic decreasing function in the damping coefficient ζ. When the linear damping factor ζ increase up to., we note that the bending contracts with decreased magnitudes and the multi-valued disappears.
13 Vibration reduction and stability of non-linear system Figs. -7 represent the eternal ecitation-response curves for primary resonance. It is evident from Fig. that the response amplitude has a continuous curve and there eist zone of multi-valued solutions. There eist jump phenomenon and the curve has unstable and stable solutions. From Fig., we observe that for increasing positive value of non-linear spring stiffness α the continuous curve is shifted downwards with decreasing region of instability. For negative values of α, the continuous curve becomes unstable and the region of multi-valued is disappeared. Figs. 5 and show that for increasing values of natural frequency ω and detuning parameter σ, respectively, the curve is shifted upwards and has increased instability region. The region of multi-valued is increased for increased natural frequency, detuning parameters. For negative value of detuning parameter σ, the continuous curve becomes stable and the region of multi-valued is disappeared as shown in Fig.. For increasing value of damping coefficient ζ, we note that the region of multi-valued is disappeared and the continuous curve has a single valued curve which is shifted downwards with increasing instability zone as shown in Fig. 7. a ζ =. ζ =. ζ =. a - σ F Fig.. Effects of the damping coefficient ζ Fig.. Ecitation-response curve of Ω ω 5 a a.5.5. F F Fig.. Effects of the non-linear spring stiffness α Fig.5. Effects of the natural frequency ω
14 M. Sayed, Y. S. Hamed and Y. A. Amer a a.. F F Fig.. Effects of the detuning parameter σ Fig.7. Effects of the damping coefficient ζ Case : The controller is activated, a, a : The frequency response equations (9) and () are nonlinear algebraic equations, which are solved numerically. The numerical results are shown in Figures -. The solid curves denote the stable solutions and the dotted curves denote the unstable solutions. These Figures, show the steady state response-frequency curve for the stability second case, where a, a in the case of simultaneous primary resonance in the presence of three-to-one internal resonance. In these Figures, we observe that the solutions is stable for negative values of σ and it has stable and unstable for positive values of σ. Fig. shows that the effect of the detuning parameter σ on the steady state amplitudes of the system and absorber. In this Figure, we observe that, the amplitudes a and a have one continuous curve, that the continuous curve of the system lies upper than the continuous curve of the absorber. For increasing ecitation force F, we note that the stability magnitudes of the system and absorber are increased as shown in Fig. 9. a a a a σ.5 Fig.. Effects of the detuning parameter σ
15 Vibration reduction and stability of non-linear system 5 Several groups of various parameters are tried out to discuss the vibration property of the system and the selections of the relative parameters are taken by virtue of Ref. []. a F = F = F = a F = F = F = - - σ Fig. 9. Effects of the ecitation amplitude F σ.. In Fig., with increase in the non-linear spring stiffness α, the vibration amplitude of the system and absorber reduces. It can be concluded that increasing the non-linear spring stiffness α can reduce the amplitude of the main mass and obtain the effect of reduction of the vibration amplitude. The system and absorber becomes unstable for negative value of non-linear spring stiffness α. Fig. shows that for increasing linear damping coefficient, we observe that the both system and absorber have decreasing magnitudes. Fig. evaluates the effectiveness of the cubic non-linear damping ζ on the amplitude reduction of the system. From the curves, it can be seen that the non-linear damping has an obvious effect on the amplitude reduction. a α =. α =. α =. a α =. α =. α =. - - σ Fig.. Effects of the non-linear parameter α -. σ.
16 M. Sayed, Y. S. Hamed and Y. A. Amer a ζ =. a ζ =. ζ =. ζ =. - - σ σ.. Fig.. Effects of the linear damping coefficient ζ a ζ =. ζ = σ.. Fig.. Effects of the cubic non-linear damping ζ 5. Conclusions The system consists of the main system and the absorber representing the vibration of many applications in machine tools, ultrasonic cutting process, subjected to eternal and parametric ecitation forces is considered and solved using the method of multiple scale perturbation. A simple and powerful effective method is demonstrated to reduce (control passively) both vibration and dynamic chaos in the non-linear system using non-linear absorber. One of the most common methods of vibration control is the dynamic absorber. Multiple scales perturbation technique is applied to determine approimate solutions of the coupled non-linear differential equations. Steady state solutions and their stability are studied for selected values of different parameters. Frequency response equations are deduced to investigate system stability. It can be seen from the results that the optimal working conditions of the system is principle parametric and internal resonance Ω ω, ω ω. From the above study the following may be concluded. (i) When the controller is deactivated. The steady state amplitude is a monotonic increasing and decreasing function to the ecitation amplitudes F, F and natural frequency ω, damping coefficient ζ, respectively.
17 Vibration reduction and stability of non-linear system 7. The zones of multi-valued and instability region are increased for large values of F.. For increasing positive value of non-linear spring stiffness α the continuous curve is shifted downwards produce hard spring with decreasing region of instability.. For negative values of α, the curve is bent to the left produce soft spring, the region of unstable is increased and the region of multi-valued is disappeared. 5. The region of multi-valued is disappeared for increasing value of damping coefficient ζ, and the continuous curve has a single valued curve which is shifted downwards.. The continuous curve becomes stable and the region of multi-valued is disappeared for negative value of detuning parameter σ. 7. (ii) When the controller is activated. The optimum working conditions for the system are when, Ω ω, ω ω since the steady state amplitude of the system is reduced to % of its maimum value. This means that the effectiveness of the absorber E a =.. The effectiveness of the absorber E a is about 5 and 7 for simultaneous primary and internal resonance Ω ω, ω ω and simultaneous resonance Ω ω, Ω ω, ω ω respectively.. For increasing ecitation force F and decreasing damping coefficient, we note that the stability magnitudes of the main system and absorber are increased.. From the curves, it can be seen that the non-linear damping has an obvious effect on the amplitude reduction of the system, which is a good agreement with Ref. []. 5. Increasing the non-linear spring stiffness α can reduce the amplitude of the main mass and obtain the effect of reduction of the vibration amplitude, which is a good agreement with Ref. [].. Numerical simulations show the system ehibits periodic motions and chaotic motions, which is a good agreement with Ref. []. In comparison with the previous work [] the authors consider the nonlinear dynamic and spring as a cubic one only. The method of averaging is used to obtain the steady state response and the system is subjected to single eternal ecitation force. The stability is studied applying bifurcation and Poincare` map. It is worth to mention that in the reported results assuming the nonlinear term is zero. In our study, the model considered in Ref. [], but subjected to eternal and parametric ecitation forces instead of an eternal only.
18 M. Sayed, Y. S. Hamed and Y. A. Amer Appendi ζ α + α5( ) = + ω ζ +ζ ( ) α = + σ+, ω α 5 ( ) =, ω α5( ) F = cos( γ ω α ( α+β = σ σ ω ω ( α+β)( ) 5 = ω 5, ζ α+α 5( ) α =ζ+ζ 5 [ ( ) ] ( σ+ ω ω 9 α5( ) α + α5( ) α5( ) 7 = + ω ω ω α5( ) α 9 = σ+ ω ω ( α+β 5 ), = ω ζ +ζ α, = + σ σ ω ωζ = ( ), = + ( ω) 7 References. Oueini SS., Nayfeh AH., Single-Mode control of a cantilever beam under principal parametric ecitation, Journal of Sound and Vibration () (999) -7.. Asfar KR., Effect of non-linearities in elastomeric material dampers on torsional vibration control, International Journal of Non-linear Mechanics 7() (99) Eissa M., Vibration Control of Non-linear Mechanical Systems Via Neutralizers, Electronic Engineering Bulletin, No., July 999, Egypt.. Eissa M., Vibration and chaos control in I.C engines subject to harmonic torque via non-linear absorbers, In. Proc of ISMV Conference, Islamabad, Pakistan,. 5. Eissa M., El-Ganaini W., Part I, Multi-absorbers for vibration control of non-linear structures to harmonic ecitations, In. Proc of ISMV Conference, Islamabad, Pakistan,.. Eissa M., El-Ganaini W., Part II, Multi-absorbers for vibration control of non-linear structures to harmonic ecitations, In. Proc of ISMV Conference, Islamabad, Pakistan,. 7. Kamel MM., Amer YA., Response of parametrically ecited one-degreeof-freedom system with non-linear damping and stiffness, Physica Scripta ().
19 Vibration reduction and stability of non-linear system 9. Song Y., Sato H., Iwata Y. and Komatsuzaki T., The response of a dynamic vibration absorber system with a parametrically ecited pendulum, Journal of Sound and Vibration 59() () Soom A., Lee M., Optimal design of linear and non-linear vibration absorbers for damped system, Journal of Vibration, Acoustic Stress, and Reliability in Design 5 (9) -9.. Jordanov IN., Cheshankov BI., Optimal design of linear and non-linear dynamic vibration absorbers, Journal of Sound and Vibration () (9) Rice H.J., Combinational instability of the non-linear vibration absorber, Journal of Sound and Vibration () (9) Shaw J., Shaw SW., Haddow AG., On the response of the non-linear vibration absorber, Journal of Non-linear Mechanics (99) -9.. Natsiavas S., Steady state oscillations and stability of non-linear dynamic vibration absorbers, Journal of Sound and Vibration 5() (99) Zhu SJ., Zheng YF., Fu YM., Analysis of non-linear dynamics of a twodegree-of-freedom vibration system with non-linear damping and non-linear spring, Journal of Sound and Vibration 7 () Lim FCN., Cartmell MP., Cardoni A., Lucas M., A preliminary investigation into optimizing the response of vibrating systems used for ultrasonic cutting, Journal of Sound and Vibration 7 () Eissa M., Amer YA., Vibration control of a cantilever beam subject to both eternal and parametric ecitation, Applied Mathematics and Computation 5 () Nayfeh AH., Resolving Controversies in the Application of the Method of Multiple Scales and the Generalized Method of Averaging, Nonlinear Dynamics (5) -.. El-bassiouny AF., Effect of non-linearities in elastomeric material dampers on torsional oscillation control, Applied Mathematics and Computation (5) Eissa M., Sayed M., A Comparison between active and passive vibration control of non-linear simple pendulum, Part I: Transversally tuned absorber n and negative G ϕ& feedback, Mathematical and Computational Applications () () Eissa M., Sayed M., A Comparison between active and passive vibration control of non-linear simple pendulum, Part II: Longitudinal tuned absorber n G ϕ&& and negative G ϕ feedback, Mathematical and Computational Applications () () 5-.. Amer YA., Vibration control of ultrasonic cutting via dynamic absorber, Chaos, Solutions & Fractals (7) Nayfeh AH., Introduction to Perturbation Techniques, John Wiley & Sons, Inc., New York, (9).
20 7 M. Sayed, Y. S. Hamed and Y. A. Amer Hamed, Y.S., EL-Ganaini, W., Kamel M. M.: Vibration suppression in ultrasonic machining described by non-linear differential equations, Journal of Mechanical Science and Technology () (9) -5. Hamed, Y.S., EL-Ganaini, W., Kamel M. M.: Vibration suppression in multitool ultrasonic machining to multi-eternal and parametric ecitations, Acta Mechanica Sinica 5 (9) 5. 5 Hamed, Y.S., EL-Ganaini, W., Kamel M. M.: Vibration reduction in ultrasonic machine to eternal and tuned ecitation forces, Applied Mathematical Modeling. (9) 5-. Received: October,
Feedback Control and Stability of the Van der Pol Equation Subjected to External and Parametric Excitation Forces
International Journal of Applied Engineering Research ISSN 973-456 Volume 3, Number 6 (8) pp. 377-3783 Feedback Control and Stability of the Van der Pol Equation Subjected to External and Parametric Excitation
More informationDYNAMICS OF AN UMBILICAL CABLE FOR UNDERGROUND BORE-WELL APPLICATIONS
DYNAMICS OF AN UMBILICAL CABLE FOR UNDERGROUND BORE-WELL APPLICATIONS 1 KANNAN SANKAR & 2 JAYA KUMAR.V.K Engineering and Industrial Services, TATA Consultancy Services, Chennai, India E-mail: sankar.kannan@tcs.com,
More informationM. Eissa * and M. Sayed Department of Engineering Mathematics, Faculty of Electronic Engineering Menouf 32952, Egypt. *
Mathematical and Computational Applications, Vol., No., pp. 5-6, 006. Association or Scientiic Research A COMPARISON BETWEEN ACTIVE AND PASSIVE VIBRATION CONTROL OF NON-LINEAR SIMPLE PENDULUM PART II:
More informationSuppression of the primary resonance vibrations of a forced nonlinear system using a dynamic vibration absorber
Suppression of the primary resonance vibrations of a forced nonlinear system using a dynamic vibration absorber J.C. Ji, N. Zhang Faculty of Engineering, University of Technology, Sydney PO Box, Broadway,
More informationα Cubic nonlinearity coefficient. ISSN: x DOI: : /JOEMS
Journal of the Egyptian Mathematical Society Volume (6) - Issue (1) - 018 ISSN: 1110-65x DOI: : 10.1608/JOEMS.018.9468 ENHANCING PD-CONTROLLER EFFICIENCY VIA TIME- DELAYS TO SUPPRESS NONLINEAR SYSTEM OSCILLATIONS
More informationActive Control and Dynamical Analysis of two Coupled Parametrically Excited Van Der Pol Oscillators
International Reereed Journal o Engineering and Science (IRJES) ISSN (Online) 39-83X, (Print) 39-8 Volume 6, Issue 7 (July 07), PP.08-0 Active Control and Dynamical Analysis o two Coupled Parametrically
More informationControl of Periodic and Chaotic Motions in a Cantilever Beam with Varying Orientation under Principal Parametric Resonance
International Journal of Control Science and Engineering 16, 6(): 3-37 DOI: 1.593/j.control.166.1 Control of Periodic and Chaotic Motions in a Cantilever Beam with Varying Orientation under Principal Parametric
More informationDesign and Analysis of a Simple Nonlinear Vibration Absorber
IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 78-1684,p-ISSN: 30-334X, Volume 11, Issue Ver. VI (Mar- Apr. 014), PP 84-90 Design and Analysis of a Simple Nonlinear Vibration Absorber
More informationIn-Plane and Out-of-Plane Dynamic Responses of Elastic Cables under External and Parametric Excitations
Applied Mathematics 5, 5(6): -4 DOI:.59/j.am.556. In-Plane and Out-of-Plane Dynamic Responses of Elastic Cables under External and Parametric Excitations Usama H. Hegazy Department of Mathematics, Faculty
More informationAdditive resonances of a controlled van der Pol-Duffing oscillator
Additive resonances of a controlled van der Pol-Duffing oscillator This paper has been published in Journal of Sound and Vibration vol. 5 issue - 8 pp.-. J.C. Ji N. Zhang Faculty of Engineering University
More informationRESPONSE OF NON-LINEAR SHOCK ABSORBERS-BOUNDARY VALUE PROBLEM ANALYSIS
Int. J. of Applied Mechanics and Engineering, 01, vol.18, No., pp.79-814 DOI: 10.478/ijame-01-0048 RESPONSE OF NON-LINEAR SHOCK ABSORBERS-BOUNDARY VALUE PROBLEM ANALYSIS M.A. RAHMAN *, U. AHMED and M.S.
More informationDifference Resonances in a controlled van der Pol-Duffing oscillator involving time. delay
Difference Resonances in a controlled van der Pol-Duffing oscillator involving time delay This paper was published in the journal Chaos, Solitions & Fractals, vol.4, no., pp.975-98, Oct 9 J.C. Ji, N. Zhang,
More informationVibrations of stretched damped beams under non-ideal boundary conditions
Sādhanā Vol. 31, Part 1, February 26, pp. 1 8. Printed in India Vibrations of stretched damped beams under non-ideal boundary conditions 1. Introduction HAKAN BOYACI Celal Bayar University, Department
More informationActive vibration control of a nonlinear beam with self- and external excitations
Shock and Vibration 20 (2013) 1033 1047 1033 DOI 10.3233/SAV-130821 IOS Press Active vibration control of a nonlinear beam with self- and external excitations J. Warminski a,, M.P. Cartmell b, A. Mitura
More informationResearch Article Approximate Super- and Sub-harmonic Response of a Multi-DOFs System with Local Cubic Nonlinearities under Resonance
Journal of Applied Mathematics Volume 212, Article ID 53148, 22 pages doi:1155/212/53148 Research Article Approximate Super- and Sub-harmonic Response of a Multi-DOFs System with Local Cubic Nonlinearities
More informationSolution of a Quadratic Non-Linear Oscillator by Elliptic Homotopy Averaging Method
Math. Sci. Lett. 4, No. 3, 313-317 (215) 313 Mathematical Sciences Letters An International Journal http://dx.doi.org/1.12785/msl/4315 Solution of a Quadratic Non-Linear Oscillator by Elliptic Homotopy
More informationStudy on Bifurcation and Chaotic Motion of a Strongly Nonlinear Torsional Vibration System under Combination Harmonic Excitations
IJCSI International Journal of Computer Science Issues Vol. Issue No March ISSN (Print): 9 ISSN (Online): 9-7 www.ijcsi.org 9 Study on Bifurcation and Chaotic Motion of a Strongly Nonlinear Torsional Vibration
More informationResonances of a Forced Mathieu Equation with Reference to Wind Turbine Blades
Resonances of a Forced Mathieu Equation with Reference to Wind Turbine Blades Venkatanarayanan Ramakrishnan and Brian F Feeny Dynamics Systems Laboratory: Vibration Research Department of Mechanical Engineering
More informationCALCULATION OF NONLINEAR VIBRATIONS OF PIECEWISE-LINEAR SYSTEMS USING THE SHOOTING METHOD
Vietnam Journal of Mechanics, VAST, Vol. 34, No. 3 (2012), pp. 157 167 CALCULATION OF NONLINEAR VIBRATIONS OF PIECEWISE-LINEAR SYSTEMS USING THE SHOOTING METHOD Nguyen Van Khang, Hoang Manh Cuong, Nguyen
More informationActive Vibration Control for A Bilinear System with Nonlinear Velocity Time-delayed Feedback
Proceedings of the World Congress on Engineering Vol III, WCE, July - 5,, London, U.K. Active Vibration Control for A Bilinear System with Nonlinear Velocity Time-delayed Feedback X. Gao, Q. Chen Abstract
More informationNONLINEAR NORMAL MODES OF COUPLED SELF-EXCITED OSCILLATORS
NONLINEAR NORMAL MODES OF COUPLED SELF-EXCITED OSCILLATORS Jerzy Warminski 1 1 Department of Applied Mechanics, Lublin University of Technology, Lublin, Poland, j.warminski@pollub.pl Abstract: The main
More informationEngineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS
Unit 2: Unit code: QCF Level: 4 Credit value: 5 Engineering Science L/60/404 OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS UNIT CONTENT OUTCOME 2 Be able to determine the behavioural characteristics of elements
More information2.034: Nonlinear Dynamics and Waves. Term Project: Nonlinear dynamics of piece-wise linear oscillators Mostafa Momen
2.034: Nonlinear Dynamics and Waves Term Project: Nonlinear dynamics of piece-wise linear oscillators Mostafa Momen May 2015 Massachusetts Institute of Technology 1 Nonlinear dynamics of piece-wise linear
More informationNON-LINEAR VIBRATION. DR. Rabinarayan Sethi,
DEPT. OF MECHANICAL ENGG., IGIT Sarang, Odisha:2012 Course Material: NON-LINEAR VIBRATION PREPARED BY DR. Rabinarayan Sethi, Assistance PROFESSOR, DEPT. OF MECHANICAL ENGG., IGIT SARANG M.Tech, B.Tech
More informationNonlinear vibration energy harvesting based on variable double well potential function
Binghamton University The Open Repository @ Binghamton (The ORB) Mechanical Engineering Faculty Scholarship Mechanical Engineering 2016 Nonlinear vibration energy harvesting based on variable double well
More informationGeneral Physics I. Lecture 12: Applications of Oscillatory Motion. Prof. WAN, Xin ( 万歆 )
General Physics I Lecture 1: Applications of Oscillatory Motion Prof. WAN, Xin ( 万歆 ) inwan@zju.edu.cn http://zimp.zju.edu.cn/~inwan/ Outline The pendulum Comparing simple harmonic motion and uniform circular
More information3.1 Centrifugal Pendulum Vibration Absorbers: Centrifugal pendulum vibration absorbers are a type of tuned dynamic absorber used for the reduction of
3.1 Centrifugal Pendulum Vibration Absorbers: Centrifugal pendulum vibration absorbers are a type of tuned dynamic absorber used for the reduction of torsional vibrations in rotating and reciprocating
More informationDynamics of a mass-spring-pendulum system with vastly different frequencies
Dynamics of a mass-spring-pendulum system with vastly different frequencies Hiba Sheheitli, hs497@cornell.edu Richard H. Rand, rhr2@cornell.edu Cornell University, Ithaca, NY, USA Abstract. We investigate
More informationChapter 2 PARAMETRIC OSCILLATOR
CHAPTER- Chapter PARAMETRIC OSCILLATOR.1 Introduction A simple pendulum consists of a mass m suspended from a string of length L which is fixed at a pivot P. When simple pendulum is displaced to an initial
More information1859. Forced transverse vibration analysis of a Rayleigh double-beam system with a Pasternak middle layer subjected to compressive axial load
1859. Forced transverse vibration analysis of a Rayleigh double-beam system with a Pasternak middle layer subjected to compressive axial load Nader Mohammadi 1, Mehrdad Nasirshoaibi 2 Department of Mechanical
More informationBifurcation of Sound Waves in a Disturbed Fluid
American Journal of Modern Physics 7; 6(5: 9-95 http://www.sciencepublishinggroup.com/j/ajmp doi:.68/j.ajmp.765.3 ISSN: 36-8867 (Print; ISSN: 36-889 (Online Bifurcation of Sound Waves in a Disturbed Fluid
More informationNonlinear dynamics of system oscillations modeled by a forced Van der Pol generalized oscillator
International Journal of Engineering and Applied Sciences (IJEAS) ISSN: 2394-3661, Volume-4, Issue-8, August 2017 Nonlinear dynamics of system oscillations modeled by a forced Van der Pol generalized oscillator
More informationVibration Analysis of a Horizontal Washing Machine, Part IV: Optimal Damped Vibration Absorber
RESEARCH ARTICLE Vibration Analysis of a Horizontal Washing Machine, Part IV: Optimal Damped Vibration Absorber Galal Ali Hassaan Department of Mechanical Design & Production, Faculty of Engineering, Cairo
More informationLinear and Nonlinear Oscillators (Lecture 2)
Linear and Nonlinear Oscillators (Lecture 2) January 25, 2016 7/441 Lecture outline A simple model of a linear oscillator lies in the foundation of many physical phenomena in accelerator dynamics. A typical
More informationClearly the passage of an eigenvalue through to the positive real half plane leads to a qualitative change in the phase portrait, i.e.
Bifurcations We have already seen how the loss of stiffness in a linear oscillator leads to instability. In a practical situation the stiffness may not degrade in a linear fashion, and instability may
More informationNON-STATIONARY RESONANCE DYNAMICS OF THE HARMONICALLY FORCED PENDULUM
CYBERNETICS AND PHYSICS, VOL. 5, NO. 3, 016, 91 95 NON-STATIONARY RESONANCE DYNAMICS OF THE HARMONICALLY FORCED PENDULUM Leonid I. Manevitch Polymer and Composite Materials Department N. N. Semenov Institute
More informationBifurcation Trees of Periodic Motions to Chaos in a Parametric, Quadratic Nonlinear Oscillator
International Journal of Bifurcation and Chaos, Vol. 24, No. 5 (2014) 1450075 (28 pages) c World Scientific Publishing Company DOI: 10.1142/S0218127414500758 Bifurcation Trees of Periodic Motions to Chaos
More information4. Complex Oscillations
4. Complex Oscillations The most common use of complex numbers in physics is for analyzing oscillations and waves. We will illustrate this with a simple but crucially important model, the damped harmonic
More informationMACROMECHANICAL PARAMETRIC AMPLIFICATION WITH A BASE-EXCITED DOUBLY CLAMPED BEAM
th International Conference on Vibration Problems Z. Dimitrovová et.al. (eds.) Lisbon, Portugal, 9 2 September 203 MACROMECHANICAL PARAMETRIC AMPLIFICATION WITH A BASE-EXCITED DOUBLY CLAMPED BEAM S. Neumeyer*,
More informationResearch Article Dynamics of an Autoparametric Pendulum-Like System with a Nonlinear Semiactive Suspension
Mathematical Problems in Engineering Volume, Article ID 57, 5 pages doi:.55//57 Research Article Dynamics of an Autoparametric Pendulum-Like System with a Nonlinear Semiactive Suspension Krzysztof Kecik
More informationApplication of a passive/active autoparametric cantilever beam absorber with PZT actuator for Duffing systems
Application of a passive/active autoparametric cantilever beam absorber with PZT actuator for Duffing systems G. Silva-Navarro* a, H.F. Abundis-Fong a and B. Vazquez-Gonzalez b a Centro de Investigación
More informationThe Effects of Machine Components on Bifurcation and Chaos as Applied to Multimachine System
1 The Effects of Machine Components on Bifurcation and Chaos as Applied to Multimachine System M. M. Alomari and B. S. Rodanski University of Technology, Sydney (UTS) P.O. Box 123, Broadway NSW 2007, Australia
More informationSTATIC AND DYNAMIC ANALYSIS OF A BISTABLE PLATE FOR APPLICATION IN MORPHING STRUCTURES
STATIC AND DYNAMIC ANALYSIS OF A BISTABLE PLATE FOR APPLICATION IN MORPHING STRUCTURES A. Carrella 1, F. Mattioni 1, A.A. Diaz 1, M.I. Friswell 1, D.J. Wagg 1 and P.M. Weaver 1 1 Department of Aerospace
More informationDETERMINATION OF THE FREQUENCY-AMPLITUDE RELATION FOR NONLINEAR OSCILLATORS WITH FRACTIONAL POTENTIAL USING HE S ENERGY BALANCE METHOD
Progress In Electromagnetics Research C, Vol. 5, 21 33, 2008 DETERMINATION OF THE FREQUENCY-AMPLITUDE RELATION FOR NONLINEAR OSCILLATORS WITH FRACTIONAL POTENTIAL USING HE S ENERGY BALANCE METHOD S. S.
More information4.5 The framework element stiffness matrix
45 The framework element stiffness matri Consider a 1 degree-of-freedom element that is straight prismatic and symmetric about both principal cross-sectional aes For such a section the shear center coincides
More informationNonlinear Stability and Bifurcation of Multi-D.O.F. Chatter System in Grinding Process
Key Engineering Materials Vols. -5 (6) pp. -5 online at http://www.scientific.net (6) Trans Tech Publications Switzerland Online available since 6//5 Nonlinear Stability and Bifurcation of Multi-D.O.F.
More informationMinimax Optimization Of Dynamic Pendulum Absorbers For A Damped Primary System
Minima Optimization Of Dynamic Pendulum Absorbers For A Damped Primary System Mohammed A. Abdel-Hafiz Galal A. Hassaan Abstract In this paper a minima optimization procedure for dynamic vibration pendulum
More informationAN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD. Mathcad Release 14. Khyruddin Akbar Ansari, Ph.D., P.E.
AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD Mathcad Release 14 Khyruddin Akbar Ansari, Ph.D., P.E. Professor of Mechanical Engineering School of Engineering and Applied Science Gonzaga University
More informationThe student will experimentally determine the parameters to represent the behavior of a damped oscillatory system of one degree of freedom.
Practice 3 NAME STUDENT ID LAB GROUP PROFESSOR INSTRUCTOR Vibrations of systems of one degree of freedom with damping QUIZ 10% PARTICIPATION & PRESENTATION 5% INVESTIGATION 10% DESIGN PROBLEM 15% CALCULATIONS
More informationNONLINEAR VIBRATIONS
NONLINEAR VIBRATIONS Prof. S. K. Dwivedy Mechanical Engineering Department Indian Institute of Technology Guwahati dwivedy@iitg.ernet.in Joint initiative of IITs and IISc Funded by MHRD Page 1 of 31 Module
More informationSolutions of Nonlinear Oscillators by Iteration Perturbation Method
Inf. Sci. Lett. 3, No. 3, 91-95 2014 91 Information Sciences Letters An International Journal http://dx.doi.org/10.12785/isl/030301 Solutions of Nonlinear Oscillators by Iteration Perturbation Method A.
More informationInvestigation of subcombination internal resonances in cantilever beams
289 Investigation of subcombination internal resonances in cantilever beams Haider N. Arafat and Ali H. Nayfeh Department of Engineering Science and Mechanics, MC 219, Virginia Polytechnic Institute and
More informationStrange dynamics of bilinear oscillator close to grazing
Strange dynamics of bilinear oscillator close to grazing Ekaterina Pavlovskaia, James Ing, Soumitro Banerjee and Marian Wiercigroch Centre for Applied Dynamics Research, School of Engineering, King s College,
More informationPassive Control of the Vibration of Flooring Systems using a Gravity Compensated Non-Linear Energy Sink
The 3 th International Workshop on Advanced Smart Materials and Smart Structures Technology July -3, 7, The University of Tokyo, Japan Passive Control of the Vibration of Flooring Systems using a Gravity
More informationDesign and Research on Characteristics of a New Vibration Isolator with Quasi-zero-stiffness Shi Peicheng1, a, Nie Gaofa1, b
International Conference on Mechanics, Materials and Structural Engineering (ICMMSE 2016 Design and Research on Characteristics of a New Vibration Isolator with Quasi-zero-stiffness Shi Peicheng1, a, Nie
More informationThe Stick-Slip Vibration and Bifurcation of a Vibro-Impact System with Dry Friction
Send Orders for Reprints to reprints@benthamscience.ae 308 The Open Mechanical Engineering Journal, 2014, 8, 308-313 Open Access The Stick-Slip Vibration and Bifurcation of a Vibro-Impact System with Dry
More informationIntroduction of Nonlinear Dynamics into a Undergraduate Intermediate Dynamics Course
Introduction of Nonlinear Dynamics into a Undergraduate Intermediate Dynamics Course Bongsu Kang Department of Mechanical Engineering Indiana University Purdue University Fort Wayne Abstract This paper
More informationResearch Article Nonlinear Response of Vibrational Conveyers with Nonideal Vibration Exciter: Superharmonic and Subharmonic Resonance
Mathematical Problems in Engineering Volume, Article ID 77543, pages doi:.55//77543 Research Article Nonlinear Response of Vibrational Conveyers with Nonideal Vibration Exciter: Superharmonic and Subharmonic
More informationThe distance of the object from the equilibrium position is m.
Answers, Even-Numbered Problems, Chapter..4.6.8.0..4.6.8 (a) A = 0.0 m (b).60 s (c) 0.65 Hz Whenever the object is released from rest, its initial displacement equals the amplitude of its SHM. (a) so 0.065
More informationChapter 23: Principles of Passive Vibration Control: Design of absorber
Chapter 23: Principles of Passive Vibration Control: Design of absorber INTRODUCTION The term 'vibration absorber' is used for passive devices attached to the vibrating structure. Such devices are made
More informationMathematical Modeling and response analysis of mechanical systems are the subjects of this chapter.
Chapter 3 Mechanical Systems A. Bazoune 3.1 INRODUCION Mathematical Modeling and response analysis of mechanical systems are the subjects of this chapter. 3. MECHANICAL ELEMENS Any mechanical system consists
More informationModelling of lateral-torsional vibrations of the crank system with a damper of vibrations
Modelling of lateral-torsional vibrations of the crank system with a damper of vibrations Bogumil Chiliński 1, Maciej Zawisza 2 Warsaw University of Technology, Institute of Machine Design Fundamentals,
More informationImproving convergence of incremental harmonic balance method using homotopy analysis method
Acta Mech Sin (2009) 25:707 712 DOI 10.1007/s10409-009-0256-4 RESEARCH PAPER Improving convergence of incremental harmonic balance method using homotopy analysis method Yanmao Chen Jike Liu Received: 10
More informationA FIELD METHOD FOR SOLVING THE EQUATIONS OF MOTION OF EXCITED SYSTEMS UDC : (045) Ivana Kovačić
FACTA UNIVERSITATIS Series: Mechanics, Automatic Control and Robotics Vol.3, N o,, pp. 53-58 A FIELD METHOD FOR SOLVING THE EQUATIONS OF MOTION OF EXCITED SYSTEMS UDC 534.:57.98(45) Ivana Kovačić Faculty
More informationAssignment 6. Using the result for the Lagrangian for a double pendulum in Problem 1.22, we get
Assignment 6 Goldstein 6.4 Obtain the normal modes of vibration for the double pendulum shown in Figure.4, assuming equal lengths, but not equal masses. Show that when the lower mass is small compared
More informationFigure 1: Schematic of ship in still water showing the action of bouyancy and weight to right the ship.
MULTI-DIMENSIONAL SYSTEM: In this computer simulation we will explore a nonlinear multi-dimensional system. As before these systems are governed by equations of the form x 1 = f 1 x 2 = f 2.. x n = f n
More information2:2:1 Resonance in the Quasiperiodic Mathieu Equation
Nonlinear Dynamics 31: 367 374, 003. 003 Kluwer Academic Publishers. Printed in the Netherlands. ::1 Resonance in the Quasiperiodic Mathieu Equation RICHARD RAND Department of Theoretical and Applied Mechanics,
More informationTuning TMDs to Fix Floors in MDOF Shear Buildings
Tuning TMDs to Fix Floors in MDOF Shear Buildings This is a paper I wrote in my first year of graduate school at Duke University. It applied the TMD tuning methodology I developed in my undergraduate research
More informationEffects of viscosity and varying gravity on liquid sloshing in a carrier subjected to external excitations
Int. J. Dynam. Control (204) 2:52 532 DOI 0.007/s40435-04-0072-y Effects of viscosity and varying gravity on liquid sloshing in a carrier subjected to external excitations Liming Dai Xiaojie Wang Received:
More information1769. On the analysis of a piecewise nonlinear-linear vibration isolator with high-static-low-dynamic-stiffness under base excitation
1769. On the analysis of a piecewise nonlinear-linear vibration isolator with high-static-low-dynamic-stiffness under base excitation Chun Cheng 1, Shunming Li 2, Yong Wang 3, Xingxing Jiang 4 College
More informationSubharmonic Oscillations and Chaos in Dynamic Atomic Force Microscopy
Subharmonic Oscillations and Chaos in Dynamic Atomic Force Microscopy John H. CANTRELL 1, Sean A. CANTRELL 2 1 NASA Langley Research Center, Hampton, Virginia 23681, USA 2 NLS Analytics, LLC, Glencoe,
More information1 Simple Harmonic Oscillator
Physics 1a Waves Lecture 3 Caltech, 10/09/18 1 Simple Harmonic Oscillator 1.4 General properties of Simple Harmonic Oscillator 1.4.4 Superposition of two independent SHO Suppose we have two SHOs described
More informationChapter 2: Complex numbers
Chapter 2: Complex numbers Complex numbers are commonplace in physics and engineering. In particular, complex numbers enable us to simplify equations and/or more easily find solutions to equations. We
More informationInvestigation of Coupled Lateral and Torsional Vibrations of a Cracked Rotor Under Radial Load
NOMENCLATURE Investigation of Coupled Lateral and Torsional Vibrations of a Cracked Rotor Under Radial Load Xi Wu, Assistant Professor Jim Meagher, Professor Clinton Judd, Graduate Student Department of
More information19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 NONLINEAR DYNAMICS IN PARAMETRIC SOUND GENERATION
9 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, -7 SEPTEMBER 7 NONLINEAR DYNAMICS IN PARAMETRIC SOUND GENERATION PACS: 43.5.Ts, 43.5.+y V.J. Sánchez Morcillo, V. Espinosa, I. Pérez-Arjona and J. Redondo
More informationMODELLING OF VIBRATION WITH ABSORBER
Journal of Machine Engineering, Vol. 10, No.4, 2010 mumerical modelling, Simulink, vibration, machine, absorber Jiří VONDŘICH 1 Evžen THÖNDE 1 Slavomír JIRKŮ 1 MODEING OF VIBRATION WITH ABSORBER Machine
More informationIntroduction to Mechanical Vibration
2103433 Introduction to Mechanical Vibration Nopdanai Ajavakom (NAV) 1 Course Topics Introduction to Vibration What is vibration? Basic concepts of vibration Modeling Linearization Single-Degree-of-Freedom
More informationHardening nonlinearity effects on forced vibration of viscoelastic dynamical systems to external step perturbation field
Int. J. Adv. Appl. Math. and Mech. 3(2) (215) 16 32 (ISSN: 2347-2529) IJAAMM Journal homepage: www.ijaamm.com International Journal of Advances in Applied Mathematics and Mechanics Hardening nonlinearity
More informationSecond-Order Linear Differential Equations C 2
C8 APPENDIX C Additional Topics in Differential Equations APPENDIX C. Second-Order Homogeneous Linear Equations Second-Order Linear Differential Equations Higher-Order Linear Differential Equations Application
More informationHopf Bifurcation Analysis and Approximation of Limit Cycle in Coupled Van Der Pol and Duffing Oscillators
The Open Acoustics Journal 8 9-3 9 Open Access Hopf ifurcation Analysis and Approximation of Limit Cycle in Coupled Van Der Pol and Duffing Oscillators Jianping Cai *a and Jianhe Shen b a Department of
More informationAn Analysis Technique for Vibration Reduction of Motor Pump
An Analysis Technique for Vibration Reduction of Motor Pump Young Kuen Cho, Seong Guk Kim, Dae Won Lee, Paul Han and Han Sung Kim Abstract The purpose of this study was to examine the efficiency of the
More informationTHE CRITICAL VELOCITY OF A MOVING TIME-HORMONIC LOAD ACTING ON A PRE-STRESSED PLATE RESTING ON A PRE- STRESSED HALF-PLANE
THE CRITICAL VELOCITY OF A MOVING TIME-HORMONIC LOAD ACTING ON A PRE-STRESSED PLATE RESTING ON A PRE- STRESSED HALF-PLANE Surkay AKBAROV a,b, Nihat LHAN (c) a YTU, Faculty of Chemistry and Metallurgy,
More informationTORSION PENDULUM: THE MECHANICAL NONLINEAR OSCILLATOR
TORSION PENDULUM: THE MECHANICAL NONLINEAR OSCILLATOR Samo Lasič, Gorazd Planinšič,, Faculty of Mathematics and Physics University of Ljubljana, Slovenija Giacomo Torzo, Department of Physics, University
More informationEstimation Of Linearised Fluid Film Coefficients In A Rotor Bearing System Subjected To Random Excitation
Estimation Of Linearised Fluid Film Coefficients In A Rotor Bearing Sstem Subjected To Random Ecitation Arshad. Khan and Ahmad A. Khan Department of Mechanical Engineering Z.. College of Engineering &
More informationTheory and Practice of Rotor Dynamics Prof. Rajiv Tiwari Department of Mechanical Engineering Indian Institute of Technology Guwahati
Theory and Practice of Rotor Dynamics Prof. Rajiv Tiwari Department of Mechanical Engineering Indian Institute of Technology Guwahati Module - 7 Instability in Rotor Systems Lecture - 2 Fluid-Film Bearings
More informationThursday, August 4, 2011
Chapter 16 Thursday, August 4, 2011 16.1 Springs in Motion: Hooke s Law and the Second-Order ODE We have seen alrealdy that differential equations are powerful tools for understanding mechanics and electro-magnetism.
More informationParametrically Excited Vibration in Rolling Element Bearings
Parametrically Ecited Vibration in Rolling Element Bearings R. Srinath ; A. Sarkar ; A. S. Sekhar 3,,3 Indian Institute of Technology Madras, India, 636 ABSTRACT A defect-free rolling element bearing has
More informationJournal of Sound and Vibration
Journal of Sound and Vibration 330 (2011) 1 8 Contents lists available at ScienceDirect Journal of Sound and Vibration journal homepage: www.elsevier.com/locate/jsvi Rapid Communications Enhanced passive
More informationAutoparametric Resonance of Relaxation Oscillations
CHAPTER 4 Autoparametric Resonance of Relaation Oscillations A joint work with Ferdinand Verhulst. Has been submitted to journal. 4.. Introduction Autoparametric resonance plays an important part in nonlinear
More informationLecture 3 : Bifurcation Analysis
Lecture 3 : Bifurcation Analysis D. Sumpter & S.C. Nicolis October - December 2008 D. Sumpter & S.C. Nicolis General settings 4 basic bifurcations (as long as there is only one unstable mode!) steady state
More informationVTU-NPTEL-NMEICT Project
VTU-NPTEL-NMEICT Project Progress Report The Project on Development of Remaining Three Quadrants to NPTEL Phase-I under grant in aid NMEICT, MHRD, New Delhi SME Name : Course Name: Type of the Course Module
More informationVibration analysis based on time-frequency analysis with a digital filter: Application to nonlinear system identification
Vibration analysis based on time-frequency analysis with a digital filter: Application to nonlinear system identification Yoshiaki ITOH 1 ; Taku IMAZU 2 ; Hiroki NAKAMURA 3 ; Toru YAMAZAKI 4 1 Kanagawa
More informationENGINEERING MECHANICS 2012 pp Svratka, Czech Republic, May 14 17, 2012 Paper #6
. 18 m 12 th International Conference ENGINEERING MECHANICS 12 pp. 255 261 Svratka, Czech Republic, May 14 17, 12 Paper #6 RESONANCE BEHAVIOUR OF SPHERICAL PENDULUM INFLUENCE OF DAMPING C. Fischer, J.
More informationAA 242B / ME 242B: Mechanical Vibrations (Spring 2016)
AA 242B / ME 242B: Mechanical Vibrations (Spring 206) Solution of Homework #3 Control Tab Figure : Schematic for the control tab. Inadequacy of a static-test A static-test for measuring θ would ideally
More informationAPPROXIMATE ANALYTICAL SOLUTIONS TO NONLINEAR OSCILLATIONS OF NON-NATURAL SYSTEMS USING HE S ENERGY BALANCE METHOD
Progress In Electromagnetics Research M, Vol. 5, 43 54, 008 APPROXIMATE ANALYTICAL SOLUTIONS TO NONLINEAR OSCILLATIONS OF NON-NATURAL SYSTEMS USING HE S ENERGY BALANCE METHOD D. D. Ganji, S. Karimpour,
More informationMATHEMATICAL MODEL OF DYNAMIC VIBRATION ABSORBER-RESPONSE PREDICTION AND REDUCTION
ANNALS of Faculty Engineering Hunedoara International Journal of Engineering Tome XIV [2016] Fascicule 1 [February] ISSN: 1584-2665 [print; online] ISSN: 1584-2673 [CD-Rom; online] a free-access multidisciplinary
More informationTheory and Practice of Rotor Dynamics Prof. Rajiv Tiwari Department of Mechanical Engineering Indian Institute of Technology Guwahati
Theory and Practice of Rotor Dynamics Prof. Rajiv Tiwari Department of Mechanical Engineering Indian Institute of Technology Guwahati Module - 7 Instability in rotor systems Lecture - 4 Steam Whirl and
More informationIntroduction to Vibration. Professor Mike Brennan
Introduction to Vibration Professor Mie Brennan Introduction to Vibration Nature of vibration of mechanical systems Free and forced vibrations Frequency response functions Fundamentals For free vibration
More informationOptimal Location of an Active Segment of Magnetorheological Fluid Layer in a Sandwich Plate
Acta Montanistica Slovaca Ročník 16 (2011), číslo 1, 95-100 Optimal Location of an Active Segment of Magnetorheological Fluid Layer in a Sandwich Plate Jacek Snamina 1 Abstract: In the present study a
More informationChapter 14. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson
Chapter 14 Periodic Motion PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Exam 3 results Class Average - 57 (Approximate grade
More information