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Relevant bibliographies by topics / Suspension geometry

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Academic literature on the topic 'Suspension geometry'

Author: Grafiati

Published: 4 June 2021

Last updated: 9 February 2022

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Journal articles on the topic "Suspension geometry"

1

Kao, M. J., C. C. Yu, H. Chang, T. T. Tsung, and H. M. Lin. "Suspension Geometry Measuring." Journal of Physics: Conference Series 48 (October 1, 2006): 255–58. http://dx.doi.org/10.1088/1742-6596/48/1/047.

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Lee, Un Koo. "Active Geometry Control Suspension." ATZ worldwide 112, no. 11 (November 2010): 4–9. http://dx.doi.org/10.1007/bf03225054.

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Lee, Un Koo. "Active Geometry Control Suspension." ATZ - Automobiltechnische Zeitschrift 111, no. 2 (February 2009): 90–96. http://dx.doi.org/10.1007/bf03222049.

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Bo, Win, Khin Maung Zaw, and Kyaw Kyaw. "Investigation on the Existing Geometry of Pathein Suspension Bridge." International Journal of Trend in Scientific Research and Development Volume-2, Issue-6 (October 31, 2018): 118–24. http://dx.doi.org/10.31142/ijtsrd18436.

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Sharp, R. S. "Variable geometry active suspension for cars." Computing & Control Engineering Journal 9, no. 5 (October 1, 1998): 217–22. http://dx.doi.org/10.1049/cce:19980505.

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Belkhode, P. N., P. V. Washimkar, and M. S. Dhande. "Predication of Steering Geometry of Front Suspension using Experimental Data Based Model." International Journal of Engineering and Technology 2, no. 6 (2010): 543–46. http://dx.doi.org/10.7763/ijet.2010.v2.179.

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Nurdin, Irwan, Idris Yaacob Iskandar, M. Rafie Johan, and Bee Chin Ang. "Characterization and Stability Monitoring of Maghemite Nanoparticle Suspensions." Advanced Materials Research 576 (October 2012): 398–401. http://dx.doi.org/10.4028/www.scientific.net/amr.576.398.

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Maghemite nanoparticle suspensions were synthesized using a co-precipitation method and characterized by a variety of techniques including XRD, TEM, magnetic measurement, DLS, and zeta potential. The stability of the suspension was monitored by measuring the particle size distribution using DLS over a period of two months. The diffraction pattern from XRD measurement confirmed that the particles were maghemite with an average crystallite size of 9.4 nm. TEM observations and analyses showed that the geometry of maghemite nanoparticles were nearly spherical with a mean physical diameter of 9.9 nm. The maghemite nanoparticles showed superparamagnetic behavior with saturation magnetization value of 32.20 emu/g. The mean hydrodynamic diameter of the suspension remained unchanged after two months which indicated no formation of aggregation. The hydrodynamic diameters recorded were 45.1 nm and 48.4 nm, respectively. Additionally, lack of sedimentation indicated that the suspension was stable. The suspension’s zeta potential values were 41.5 mV and 40.4 mV for as synthesized and after two month of storage respectively.

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Klein, J., R. Schwänzl, and R. M. Vogt. "Comultiplication and suspension." Topology and its Applications 77, no. 1 (May 1997): 1–18. http://dx.doi.org/10.1016/s0166-8641(96)00103-4.

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Strickland, Neil P. "Chains on suspension spectra." Algebraic & Geometric Topology 9, no. 3 (September 2, 2009): 1681–725. http://dx.doi.org/10.2140/agt.2009.9.1681.

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Lee, S. H., U. K. Lee, and C. S. Han. "Enhancement of vehicle handling characteristics by suspension kinematic control." Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering 215, no. 2 (February 1, 2001): 197–216. http://dx.doi.org/10.1243/0954407011525584.

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In this paper, the enhancement of vehicle handling characteristics through the active kinematic control system (AKCS) is investigated. AKCS can improve the stability and ride comfort of a vehicle by automatically controlling suspension geometry in accordance with the running conditions of a vehicle. The variable roll centre suspension concept in a McPherson strut suspension is proposed, and lateral acceleration feedback control is derived to calculate the control input. The independent rear wheel steering system, which controls both rear wheels independently and actively, is also proposed. To achieve this, three suggested positions for controlling the suspension geometry are considered. The first position is between the mounting point of the lower arm of a McPherson front suspension and the vehicle body. The second position is between the mounting point of the strut and the vehicle body. The third position is between the mounting point of the lateral link of the multilink rear suspension and the vehicle body. In order to evaluate the handling performance, a 15 degrees of freedom full vehicle model is constructed using the commercial multibody analysis program ADAMS. The control inputs for integrated control of the front and rear suspensions are defined, and roll centre migration and vehicle behaviour are investigated. In step steering and double lane change manoeuvres, the simulation results demonstrate that integrated kinematic control can adjust the roll centre migration, by which the handling characteristics of the AKCS vehicle such as roll angle, lateral acceleration and yaw rate are much improved.

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Dissertations / Theses on the topic "Suspension geometry"

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Minaker, Bruce P. "Active geometry suspension for road vehicles." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 2001. http://www.collectionscanada.ca/obj/s4/f2/dsk3/ftp04/NQ59533.pdf.

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Arana, Remirez Carlos. "Active variable geometry suspension for cars." Thesis, Imperial College London, 2015. http://hdl.handle.net/10044/1/41040.

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This thesis investigates the characteristics and performance of a new type of active suspension for cars through modelling, simulation, control design and experimental testing. The Series Active Variable Geometry Suspension (SAVGS) concept is first put in context by reviewing the history and current trends in automotive suspensions. Its potential is then critically evaluated and work is carried out to maximise its performance for various suspension functions. A multi-model multi-software modelling and simulation approach is followed throughout the thesis in order to cross-check and substantiate simulation results in the absence of experimental data. The simpler linear models are used to inform the selection of suitable parameter sets for the case studies, to synthesise control systems and to qualitatively validate the more complex, nonlinear multi-body models. The latter are developed as a platform to virtually test the system and its control algorithms. When possible, these tests are based on standard open-loop test manoeuvres and on standardised external disturbances. The SAVGS-retrofitted suspension displays a very nonlinear behaviour, which is at the same time a liability and an opportunity from the point of view of control. Nevertheless, different linear control techniques are effectively applied to improve various suspension functions: PIDs are applied to the lower frequency suspension functions such as mitigation of chassis attitude motions, and the H∞ framework is applied to the higher frequency suspension functions such as comfort and road holding enhancement. In all cases, a cascade control approach is employed, and mechanisms are implemented to ensure that physical and design actuator constraints are always respected. This thesis also covers the design and construction of a quarter-car experimental test rig facility. Step-by-step recommendations for its refinement as well as a testing plan are also outlined.

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Bujalski, Waldemar. "Three phase mixing : studies of geometry, viscosity and scale." Thesis, University of Birmingham, 1986. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.323109.

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One-, two- and three-phase mixing systems have been extensively studied. The experiments were performed in a range of standard (baffled) vessel geometries of diameter varying between 0.22 - 1.83 m. Rushton disc turbines and mixed flow impellers (both pumping directions) were fully investigated. Water and glucose solution (~ - 120 mPas) were employed. For single phase systems, the work has shown that the power number of disc turbines depends on disc thickness and scale of vessel. For the mixed flow agitators the power number is dependent upon the blade thickness and (D/T) ratio. Correlations enabling the ungassed power number to be calculated as a function of these parameters are given. For gassed systems, the power drawn by each type of impeller is explained by local impeller hyarodynamics (cavity structure) and the bulk flow pattern. The fiooding-Ioading transition (NF) and the complet~ dispersion condition (NeD) have also been studied. A large mixed flow impeller (6MFU45 ; D - T/2) with a large ring sparger is the most energy efficient at NF and NCD speeds as compared with the other geometries studied and correlations enabling the prediction of NF and NCD for all geometries studied are presented. Hold-up correlations are also given for each impeller firstly as a function of specific energy dissipation rate and superficial gas velocity and secondly as' a function of agitator speed and volumetric gassing rate. For each impeller, each method is equally good statistically for scale-up but the latter is more explicit. All impellers give approximately the same hold-up under equal specific power inputs and superficial gas velocity but there are small but statistically significant differences. These differences are discussed. For solid-liquid systems, correlations in the literature for the calculation of the minimum speed to just suspend solids, NJS ' are tested for each system geometry with glass Ballotini particles. The correlation proposed by Chapman et al. is shown to fit the present experimental data best. The specific power input per unit mass (ET)JS - constant, is proposed as a scale-up criterion for solids suspension. Large 6MFD45 (D - T/2) is the most energy efficient for suspension but 6MFU45 (D - T/2) is only slightly worse. In the three-phase mixing systems, the 6MFD 45 , D - T/2, is most energy efficient for solid suspension (ET)JSg' at low gassing rates (up to 1 vvm) but exhibits large flow pattern and torque fluctuations. Above _ 1 vvm, 6MFU45 (D = T/2) becomes the most energy efficient for solid suspension. In addition the minimum impeller speed for solid suspension NJSg for this impeller is almost independent of gassing rate and gives very stable flow patterns and torque. output throughout the whole gassing range. Again (eT)JSg - const is the recommended scale-up criterion for solids suspension under gassed conditions. Large (D - T/2) impellers are found to be more energy efficient and correlations for predicting N 45 45 . JSg for 6DT. 6MFD and 6MFU are obta~ned. Increase in liquid viscosity has a rather small effect on gas dispersion. Up to 120 mPas: (N) Q:I (N ) and (N ) Q:I F viscous F water CD viscous (NCD) water uO.06 On the other hand, viscosity has a significant effect on NJS and 3 to 5 times more energy is required for solid suspension at 120 ,mPas.

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Ness, Christopher John. "Suspension rheology and extrusion : a discrete element method study." Thesis, University of Edinburgh, 2016. http://hdl.handle.net/1842/20392.

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A suspension is a fully saturated mixture of discrete solid particles and interstitial liquid. Examples of suspensions include pastes, slurries, cement, food-spreads, drilling fluids and some geophysical flows. The present work focusses on granular (as opposed to colloidal) suspensions, which we define as those for which the thermal motion of the solid particles is negligible. Despite such ubiquity in industry and nature, our understanding of the mechanical properties of suspensions lags behind that of their constituent solid and liquids. In this thesis, the discrete element method is used to simulate suspension flow in shear, capillary and constriction geometries, mapping and characterising the fundamental flow, or rheological, regimes. As a starting point (Chapter 2), we consider an established regime map for dry granular materials, appropriate for flows of sand, grains and dry debris. Taking guidance from shear flow simulations that consider the lubricating effect of an interstitial liquid, we recast the regime map for a general suspension, elucidating flows comparable to the dry material or to a viscous liquid, dependent on the shear rate, liquid viscosity and particle stiffness. We give an account of the microstructural traits associated with each regime. Motivated by recent groundbreaking theoretical, computational and experimental work, we incorporate the emerging picture of frictional shear thickening into our regime map (Chapter 3). Our shear flow simulations capture the shear thickening behaviour and demonstrate that it may, in principle, occur in any of the identified flow regimes. Our simulations of time-dependent shear flows (Chapter 4), specifically flow reversal, provide a detailed micro-mechanical explanation of a longstanding and previously unexplained experimental finding, guiding future experimentalists in decomposing the particle and liquid contributions to the viscosity of any suspension. Indeed, the findings have already been exploited in the devising of an experimental protocol that has successfully proven the dominance of particle contacts in driving shear thickening. We next consider suspension flow in a microchannel (Chapter 5), finding that the identified shear flow regimes are locally applicable to flows in complex geometries under inhomogeneous stress conditions only when the local mean shear rate exceeds temporal velocity fluctuations. A more comprehensive description is therefore required to fully characterise the flow behaviour in this geometry. Finally (Chapter 6), we simulate pressure driven suspension flow through a constriction geometry, observing highly inhomogeneous stress distributions and velocity profiles. The roles of particle and fluid properties are considered in the context of an industrial paste extrusion process.

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Arensen, Bruce (Bruce Edward). "Design and analysis of the front suspension geometry and steering system for a solar electric vehicle." Thesis, Massachusetts Institute of Technology, 2014. http://hdl.handle.net/1721.1/92663.

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Thesis: S.B., Massachusetts Institute of Technology, Department of Mechanical Engineering, 2014.
Cataloged from PDF version of thesis.
Includes bibliographical references (page 43).
A study on the design of the front suspension geometry and steering system to be used in a solar electric vehicle. The suspension geometry utilizes a double wishbone design that is optimized to fit in the space constraints of the vehicle. The steering system consists of a rack and pinion connected through tie rods to the steering knuckles, largely optimized based on the space within the vehicle. The final suspension geometry consists of upper and lower wishbone lengths of 4.25 inches and 3.75 inches, respectively. This system is optimized to maintain a proper camber angle and minimize scrub due to track distance changes throughout the travel of the suspension. The geometry of the steering system is designed to fit in the vehicle while achieving a near- Ackermann steering condition. The steering knuckle and steering rack extenders, both made out of Aluminum 6061-T6, are designed based off of this geometry and are optimized for weight and machinability.
by Bruce Arensen.
S.B.

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Vávra, Radek. "Optimalizace kyvadlové nápravy automobilu." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2015. http://www.nusl.cz/ntk/nusl-231769.

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This thesis is concerned with the design of Škoda 130 RS rear Semi-Trailing Arm Suspension and fixtures on the body. The main requirement of this thesis is to reduce weight of suspension. It is carried out the kinematic analysis and optimization of the kinematic. The construction part of this thesis provides a design of suspension based on the analysis of forces acting on the car wheel. Last part of the thesis includes of new rear suspension stress analysis.

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Martínek, Tomáš. "Zavěšení kol sportovního automobilu." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2011. http://www.nusl.cz/ntk/nusl-229639.

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This thesis deals with design of front and rear suspension of single-seater sports car. Design and optimization of geometrical parametres of axles is followed after theoretical introduction. Another section is concerned with calculation of the vehicle suspension and design of the steering. The construction of individual components is described in the final section.

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Zubíček, David. "Návrh podvozkové skupiny vozu Formule Student." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2016. http://www.nusl.cz/ntk/nusl-254225.

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Diploma thesis deals with comparison of different types of tyres destined for Formula Student vehicle. Comparison is from view of chosen characteristics and from view of simulations for one lap. Thesis deals with kinematics design of suspension according to chosen tyre and according to improvement of car ability of monopost Dragon 6

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Dvořák, Martin. "Měření geometrie a kinematiky zavěšení s využitím optických scannerů Tritop a Atos." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2012. http://www.nusl.cz/ntk/nusl-230350.

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The diploma thesis is focused to possibility utilizing of optical scanners TRITOP and ATOS for set up geometry of wheels. In background research are described the most important parameters of wheel suspension and devices for measuring these parameters. Practical part is concerned with progression of measurement, results and with determination coordinates of kinematic points. These points are made 3D model of forward and backward suspension wheels. This model helps to make kinematic characteristics and its progression due to attitude of wheel. In last part is described possibility to utilizing of optical scanner ATOS to common measurement of geometry wheels.

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Vojtěšek, Aleš. "Měření odklonu kola během jízdy." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2015. http://www.nusl.cz/ntk/nusl-231779.

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The subject of this master's thesis is design measurement and measure change wheel camber angle during driving. For this task were used parts from Corrsys-Datron and remaining elements needed to be manufactured. With complete system measurements were done and outputs data were displayed by Matlab and evaluated. Based on data evaluation is possible exactly determine relative position of the wheel to the road surface and to the body of vehicle.

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Books on the topic "Suspension geometry"

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Dixon, John C. Suspension geometry and computation. Chichester, U.K: Wiley, 2009.

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Heimbecher, John. Suspension geometry and design. [S.l.]: DaimlerChrysler, 1998.

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Dixon, John C. Suspension geometry and computation. Hoboken, N.J: Wiley, 2009.

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Dixon, John C. Suspension Geometry and Computation. Wiley & Sons, Incorporated, John, 2009.

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Book chapters on the topic "Suspension geometry"

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Deep, Mrinal, Pranav Upadhyay, and Pikesh Bansal. "Design and Optimization of Suspension Geometry." In Lecture Notes in Mechanical Engineering, 651–58. Singapore: Springer Singapore, 2020. http://dx.doi.org/10.1007/978-981-15-8704-7_80.

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Gáspár, Péter, Zoltán Szabó, József Bokor, and Balázs Németh. "Control of the Variable-Geometry Suspension." In Robust Control Design for Active Driver Assistance Systems, 187–98. Cham: Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-46126-7_8.

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Németh, B., D. Fényes, and P. Gáspár. "Control of a variable-geometry suspension as independent wheel steering." In Advanced Vehicle Control AVEC’16, 261–68. CRC Press/Balkema, P.O. Box 11320, 2301 EH Leiden, The Netherlands, e-mail: Pub.NL@taylorandfrancis.com, www.crcpress.com – www.taylorandfrancis.com: Crc Press, 2016. http://dx.doi.org/10.1201/9781315265285-42.

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Minaker, Bruce, and Ronald J. Anderson. "Modelling the Dynamics of a Vehicle with Active Geometry Suspension." In The Dynamics of Vehicles on Roads and on Tracks, 716–27. London: CRC Press, 2021. http://dx.doi.org/10.1201/9781003210924-59.

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Zhang, B. "Heat Leak Analysis on a Cryostat Suspension System with Complex Geometry." In Advances in Cryogenic Engineering, 613–18. Boston, MA: Springer US, 1994. http://dx.doi.org/10.1007/978-1-4615-2522-6_74.

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Alsayed, Ahmed M., Yilong Han, and Arjun G. Yodh. "Melting and Geometric Frustration in Temperature-Sensitive Colloids." In Microgel Suspensions, 229–81. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA, 2011. http://dx.doi.org/10.1002/9783527632992.ch10.

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Waldron, K. J., S. M. Song, S. L. Wang, and J. Vohnout. "Mechanical and Geometric Design of the Adaptive Suspension Vehicle." In Theory and Practice of Robots and Manipulators, 295–306. Boston, MA: Springer US, 1985. http://dx.doi.org/10.1007/978-1-4615-9882-4_32.

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Dronawat, Sundeep N., C. Kurt Svihla, and Thomas R. Hanley. "Effect of Impeller Geometry on Gas-Liquid Mass Transfer Coefficients in Filamentous Suspensions." In Biotechnology for Fuels and Chemicals, 363–73. Totowa, NJ: Humana Press, 1997. http://dx.doi.org/10.1007/978-1-4612-2312-2_32.

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"Optimal control and construction design of variable-geometry suspension systems." In The Dynamics of Vehicles on Roads and Tracks, 624–29. CRC Press, 2016. http://dx.doi.org/10.1201/b21185-65.

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Stygar Lopes, Marina. "Colloidal Stability of Cellulose Suspensions." In Colloids - Types, Preparation and Applications [Working Title]. IntechOpen, 2020. http://dx.doi.org/10.5772/intechopen.94490.

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Cellulose is the most abundant natural compound in nature and the main component of the cell wall of plants. It is a linear polymer with a high degree of polymerization, responsible for most of the properties of wood. Colloidal phenomena are often used in various industrial production processes. Suspended cellulose, used worldwide in the paper and cellulose industries, with regard to stability, has a high tendency to aggregate and form clots. The different interactions between the dispersed phase and the dispersion phase are one of the critical points in the study of the behavior and stability of colloids. Cellulose is no different, as several studies seek to improve the colloidal stability of cellulose in aqueous media by observing the specific characteristics of the colloid, such as its geometry, mass and area/volume ratio, and the possible interactions between particles that make up the cellulose dispersion in order to understand and control colloidal stability. Therefore, the objective of this chapter is to define the main characteristics of colloids, to classify them, to present the main methods of preparation, to address important aspects about colloid stability and the colloidal stability of cellulose.

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Conference papers on the topic "Suspension geometry"

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Sharp, R. S. "Variable geometry active suspension." In IEE Colloquium on Industrial Automation and Control: Applications in the Automotive Industry. IEE, 1998. http://dx.doi.org/10.1049/ic:19980213.

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Silva, R. C., M. A. A. Nunes, A. B. S. Oliveira, and G. O. Andrade. "Estimation of the Geometric Parameters of a Front Double Wishbone Suspension Based on Geometry Formulation." In ASME 2015 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2015. http://dx.doi.org/10.1115/imece2015-50012.

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Vehicle suspension stands out as an important subsystem, which allows vertical compliance to the wheels following an uneven road; keeps the proper steer and camber attitudes, resist roll of the chassis and provides comfort for passengers. The suspension subsystem needs to comply with stability, handling and optimum steering based on an appropriate suspension geometry. Nowadays, the use of simulation software in automotive design has increased. However, the cost and complexity of such software can make them unavailable to those working in the domain, especially the young designers working in vehicle’s student competition (Baja SAE®). Thus, this paper aims to propose a methodology for assessing a frontal Double Wishbone suspension, which is based on a set of analytical equations implemented computationally at Matlab®. The formulae are developed considering simple concepts of algebra, trigonometry and geometry. The input data are the Cartesian coordinates (x, y, z) of predefined points, which are obtained from the CAD design and the bound/rebound travel. The main results are the simple analytical formulae, for the most important suspension’s geometric parameters: caster, camber and toe angles. These analytical results are validated with MSC ADAMS®, particularly its add-on specialized for the automotive industry ADAMS/Car®, showing good agreement.

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Powell, Andre, Joseph Henry, and Patrick Fitzhorn. "As-Assembled Suspension Geometry Measurement using Photogrammetry." In Motorsports Engineering Conference & Exposition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2006. http://dx.doi.org/10.4271/2006-01-3618.

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Evangelou, Simos A. "Control of motorcycles by variable geometry rear suspension." In Control (MSC). IEEE, 2010. http://dx.doi.org/10.1109/cca.2010.5611082.

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Nemeth, Balazs, and Peter Gaspar. "Variable-geometry suspension design in driver assistance systems." In 2013 European Control Conference (ECC). IEEE, 2013. http://dx.doi.org/10.23919/ecc.2013.6669551.

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Kumar, G. Naga Siva, Sushanta K. Mitra, and Subir Bhattacharjee. "Dielectrophoretic Mixing With Novel Electrode Geometry." In ASME 2009 Fluids Engineering Division Summer Meeting. ASMEDC, 2009. http://dx.doi.org/10.1115/fedsm2009-78260.

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Electrokinetic mixing of analytes at micro-scale is important in several biochemical applications like cell activation, DNA hybridization, protein folding, immunoassays and enzyme reactions. This paper deals with the modeling and numerical simulation of micromixing of two different types of colloidal suspensions based on principle of dielectrophoresis (DEP). A mathematical model is developed based on Laplace, Navier-Stokes, and convection-diffusion-migration equations to calculate electric field, velocity, and concentration distributions, respectively. Mixing of two colloidal suspensions is simulated in a three-dimensional computational domain using finite element analysis considering dielectrophoretic, gravitational and convective (advective)–diffusive forces. Phase shifted AC signal is applied to the alternating electrodes for achieving the mixing of two different colloidal suspensions. The results indicate that the electric field and DEP forces are maximum at the edges of the electrodes and become minimum elsewhere. As compared to curved edges, straight edges of electrodes have lower electric field and DEP forces. The results also indicate that DEP force decays exponentially along the height of the channel. The effect of DEP forces on the concentration profile is studied. It is observed that, the concentration of colloidal particles at the electrodes edges is very less compared to elsewhere. Mixing of two colloidal suspensions due to diffusion is observed at the interface of the two suspensions. The improvement in mixing after applying the repulsive DEP forces on the colloidal suspension is observed. Most of the mixing takes place across the slant edges of the triangular electrodes. The effect of electrode pairs and the mixing length on degree of mixing efficiency are also observed.

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Yasuda, Kazunori, and Noriyasu Mori. "Fiber Orientation and Concentration Distribution in a Concentrated Suspension Flow Through a Complex Geometry." In ASME/JSME 2003 4th Joint Fluids Summer Engineering Conference. ASMEDC, 2003. http://dx.doi.org/10.1115/fedsm2003-45778.

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Distributions of fiber orientation and fiber concentration in slit flows of concentrated suspensions were measured. Slit channels were used in the experiments: a channel with an abrupt expansion and a crank geometry with six L-shaped corners. Such channels are usually used in a polymer processing. For visualization of fibers, an index-of-refraction matching method was employed, and tracer fibers having birefringence were suspended to observe between crossed polarizers. When fibers flow through an abrupt expansion, they rapidly orient in the direction perpendicular to the flow direction near the centerline. The fiber orientation, however, returns to the flow direction in the downstream region. In the L-shaped corner, fibers randomly orient because of the decelerating flow. In the downstream region of the L-shaped corner, fiber orientation is not symmetric with respect to the centerline. This seems to result from fiber-fiber interactions in the concentrated suspension. The fiber concentration is uniform over a width of a channel except adjacent to the side wall in the concentrated suspension, while it has a maximum apart from the side wall in the dilute suspension.

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Mitchell, Wm C., Robert Simons, Timothy Sutherland, and Michael Keena-Levin. "Suspension Geometry: Theory vs. K & amp;C Measurement." In Motorsports Engineering Conference & Exposition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2008. http://dx.doi.org/10.4271/2008-01-2948.

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Lee, Sangho, Hyun Sung, and Unkoo Lee. "The Development of Active Geometry Control Suspension (AGCS) System." In SAE 2005 World Congress & Exhibition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2005. http://dx.doi.org/10.4271/2005-01-1927.

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Nemeth, Balazs, and Peter Gaspar. "Uncertainty modeling and control design of variable-geometry suspension." In 2011 IEEE 12th International Symposium on Computational Intelligence and Informatics (CINTI). IEEE, 2011. http://dx.doi.org/10.1109/cinti.2011.6108500.

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