Abstract
A magnetorheological (MR) damper is effective and economical for miscellaneous applications in automotive, mechanical, civil, and relative fields. A parameter tuning methodology independent of manual trial-and-error has received much technical interest for controlling vibrations. The present work contributes mathematical and Simulink modeling followed by MR damper design and development for vibration optimization of the single degree of freedom system. A Simulink model of an MR damper is performed on the mathematical model for vibration control, and the MR damper’s tuning parameters are experimentally investigated to control the resonance frequency. Theoretical simulated results and its experimental verification show that increasing current raises the force to control the resonance frequency in an MR damper. The present approach provides a concise and improved platform for dynamic vibration absorber in the current potential market and the highly interested control community for the development of the distinctive attributes of the MR Damper.
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Abbreviations
- A :
-
Parameter to determine the hysteresis loop in the Bouc–Wen model (dimensionless)
- c 0 :
-
Viscous damping at large velocities, Ns/m
- c 1 :
-
Dashpot used to introduce the nonlinear roll-off observed at low velocities, Ns/m
- c 2 :
-
Damper of the secondary system, Ns/m
- C 0b :
-
Constant that determines Co, Ns/m
- C 1a :
-
Constant that determines C1, Ns/m
- C 1b :
-
Constant that determines C1b, Ns/mV
- F :
-
Frequency of external force, Hz
- f d :
-
Force of damper, N
- \({F}_{o}\) :
-
Amplitude of exciting force due to eccentricity, N
- e :
-
Radial eccentricity of its cam, m
- K o :
-
Preload stiffness, N/m
- K 1 :
-
Primary (supporting) system stiffness, N/m
- K 2 :
-
Secondary (absorber) system stiffness, N/m
- K 3 :
-
Accumulator stiffness, N/m
- m :
-
Mass of eccentricity, kg
- m 1 :
-
Primary mass, kg
- m 2 :
-
Secondary (absorber) mass, kg
- z, \(\dot{z}\) :
-
Variable to depict the history dependence of applied response, Hz
- X :
-
Displacement of the damper piston, m
- \(\dot{y}\) :
-
Velocity of the damper piston, m/s
- N :
-
Wen model (dimensionless)
- x 0 :
-
Initial displacement of spring k1 associated with nominal damper force to accumulator, m
- x 1, x 2 :
-
Displacement of m1 and m2, m
- \({\ddot{x}}_{1},{\ddot{x}}_{2}\) :
-
Acceleration of m1 and m2, m/s2
- Α :
-
Scaling value for Bouc–Wen model, N/m
- α a :
-
Constant that determines α, N/m
- α b :
-
Constant that determines α, N/mV
- γ μ :
-
Parameter that determines the hysteresis loop in the Bouc–Wen model, m−2
- \({\mu }^{{\prime}}\) :
-
Mass ratio (dimensionless)
- \(\dot{u}\) :
-
Constant to govern the first-order filter, s−1
- t :
-
Time, s
- \(\omega\) :
-
Frequency of rotation, rpm
- η :
-
Constant to govern the first-order filter, s−1
- SDOF:
-
Single degree of freedom system
- DVA:
-
Dynamic vibration absorber
- MRDVA:
-
Magnetorheological dynamic vibration absorber
- TVS:
-
Transient voltage suppression
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Kumbhar, M.B., Desavale, R.G. & Kumbhar, S.G. Dynamic Characterization of MR Fluid-Based Dynamic Vibration Absorber. Arab J Sci Eng 48, 11363–11377 (2023). https://doi.org/10.1007/s13369-022-07410-3
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DOI: https://doi.org/10.1007/s13369-022-07410-3