2012
DOI: 10.1002/ls.170
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Effect of surface roughness on magneto‐hydrodynamic couple‐stress squeeze film lubrication between circular stepped plates

Abstract: In this paper, a theoretical analysis of the problem of magneto‐hydrodynamic couple‐stress squeeze film lubrication between rough circular stepped plates is presented. The modified averaged Reynolds equation is derived for the two types of one‐dimensional roughness structures, namely the radial roughness pattern and the azimuthal roughness pattern. The closed‐form expressions are obtained for the mean squeeze film pressure, load‐carrying capacity and squeeze film time. The results are presented for different o… Show more

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Cited by 12 publications
(4 citation statements)
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“…In the literature, the experimental study of circular stepped disks is not available. However, a theoretical study on magneto-hydrodynamic couple-stress squeeze film characteristics between rough circular stepped disks has been carried out by Naduvinamani et al (2012). Neglecting the effects of magneto-hydrodynamic couple stresses and rough surfaces, their integrated Reynolds equation agrees with the present lubrication equation (3) with neglecting the term: 9v s 2 r/10h i 2 .…”
Section: Industrial Lubrication and Tribologymentioning
confidence: 64%
“…In the literature, the experimental study of circular stepped disks is not available. However, a theoretical study on magneto-hydrodynamic couple-stress squeeze film characteristics between rough circular stepped disks has been carried out by Naduvinamani et al (2012). Neglecting the effects of magneto-hydrodynamic couple stresses and rough surfaces, their integrated Reynolds equation agrees with the present lubrication equation (3) with neglecting the term: 9v s 2 r/10h i 2 .…”
Section: Industrial Lubrication and Tribologymentioning
confidence: 64%
“…Figure 3 exhibits that the maximum dimensionless pressure peak (P max ) increases with increase in g. Under constant conditions of q = 0.1, L* = 0.2, Ce = 0.3, e = 0.1, l = 1.0 and b = 0.8, it is evident that P max for magnetized journal bearings obviously increase with increase in magnetic fluids supporting force (g) by about 5.5%, 16.7%, and 38.1% for g = 0.05, g = 0.1 and g = 0.2 in comparison with magnetized journal bearings without magnetic fluids supporting force (g = 0.0) respectively. This phenomenon is mainly due 2.8 3 10 24 m Ratio of width to diameter of bearing, l 1.0 Journal speed, n 2500 RPM Derivative of eccentricity ratio, _ e 0.1(q = 1.0,0.1,0.5), 0(q = 0.0) Derivative of attitude angle, _ u 130.8(q = 1.0), 130.7(q = 0.5), 129.9(q = 0.1) Magnetic fluids supporting force parameter, g 18,19 0.0, 0.05, 0.1, and 0.2 Couple-stress factor L* [20][21][22] 0.0, 0. to the magnetic fluids supporting force generated by the viscosity increase of magnetic fluids under the applied magnetic field, which increases P max . The larger the magnetic fluids supporting force parameter, the bigger maximum dimensionless pressure peak.…”
Section: Resultsmentioning
confidence: 99%
“…Equation (23) shows that the side leakage of magnetic fluids' journal bearing is determined as a resultant of two opposite effect. One is the pressure gradient ∂P=∂Z of magnetic fluids' oil film (at Z = 0.5), which is the main cause of increasing the side leakage, and the other cause is the sealing magnetic fluids' cohesion force F mz = m 0 X m H m (∂H m =∂Z) (at Z = 0.5) that reduces the side leakage.…”
Section: Parametersmentioning
confidence: 99%