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Dmitri Kopeliovich (SubsTech, Smooth Sliding)

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Hydrodynamic Bearing – Calculations and Design

Hydrodynamic Force

A body moving through a liquid experiences a resistance generated by the hydrodynamic force. Effect of hydrodynamic forces is principal for reliable and stable work of hydrodynamic bearings. Action of hydrodynamic force upon a subject moving in a fluid may be shown by example of a water skier (Fig.1). The force Ft pulls the skier horizontally. The gravity force Fg acts vertically and is directed downwards. Reaction of water on the moving ski produces the hydrodynamic force, which can be presented as a combination of the horizontal vector Fd (drug force) and vertical vector Fl (lift force). When the skier is skimming on the water surface, the forces are balanced: Fd counteracts Ft in the horizontal direction, whereas Fl counteracts Fg in the vertical direction.

water_skier

Fig.1 Hydrodynamic Force

The Fd-to-Fl ratio and their absolute values are determined by the skier speed, his weight and the wedge angle α (angle of attack). Too low towing speed and too little wedge α produce the lift force that is incapable to balance the gravity force and cause the skier to sink.

Thus for steady skiing, the three conditions are crucial:

  • Sufficient speed;
  • Sufficient wedge;
  • Sufficient amount (depth) of the liquid (water).

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Hydrodynamic Bearing

The same three conditions determine a stable work of hydrodynamic bearings. Fig.2 depicts a hydrodynamic bearing and a journal rotating in a clockwise direction. Hydrodynamic bearing is a bearing operating with hydrodynamic lubrication, in which the bearing surface is separated from the journal surface by the lubricant film generated by the journal rotation.

Journal Bearing

Fig.2 Hydrodynamic Bearing

Journal rotation causes pumping of the fluid flowing around the bearing in the direction of rotation.
The external force F displaces the journal from the bearing center. The journal surface is getting closer to the bearing surface forming a converging gap (wedge) α between the bearing and the journal surfaces. The presence of this oil wedge is indispensable to the normal operation of a hydrodynamic bearing.
The oil pressure creates a Lift Force separating the journal from the bearing surface. The Lift force counteracts the external force F. The lubricant enforced to squeeze through the gap between the bearing and journal surfaces produces the hydrodynamic friction.
The balance between the forces determines the final position of the journal: the value of minimum oil film thickness (MOFT) and the distance between the bearing and journal centers (eccentricity e). In the hydrodynamic regime, the journal “climbs” in the rotation direction at the angle φa (attitude angle).

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Reynolds Equation

A theoretical analysis of hydrodynamic lubrication was carried out by Osborne Reynolds. Lubricant pressure distribution as a function of journal speed, bearing geometry, oil clearance and lubricant viscosity is described by the Reynolds equation that is a basis for designing hydrodynamic bearings:
Reynolds Equation

Where:
h – local oil film thickness,
η – dynamic viscosity of oil,
p – local oil film pressure,
U – linear velocity of journal,
x - circumferential direction,
z - longitudinal direction.

Close form solution of the Reynolds equation can not be obtained therefore finite elements method is used to solve it.

Analytical solutions of Reynolds equation exist only for certain assumptions:

  • Sommerfeld Solution

Sommerfeld Solution

The equation is solved with the assumption that there is no lubricant flow in the axial direction (infinitely long bearing assumption).

  • Ocvirk Solution

Ocvirk solution for infinitely short bearing assumption neglects circumferential pressure gradients (first term of Reynolds equation).

Ocvirk Solution

Where:
Cr – radial clearance Cr = (D-Dj)/2,
r – bearing radius,
Dj - journal diameter,
ε - eccentricity ratio ε = e/Cr,
e - absolute bearing eccentricity,
B – bearing length,
p0 - cavitation pressure,
So - Sommerfeld number So = F Ψ²/(DBωη),
F – bearing load,
Ψ – relative bearing clearance Ψ = (D-Dj)/D,
D – bearing diameter,
η – dynamic viscosity of oil,
ω – angular speed of journal.

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Practical Applications of Reynolds Equation

The Reynolds equation is used for calculating hydrodynamic conditions of bearing operation: minimum oil film thickness, oil temperature rise, coefficient of friction, power friction loss, oil flow rate. When a bearing is being designed, theoretical simulation of hydrodynamic lubrication is performed to optimize the bearing dimensions and lubrication conditions.

Here are three examples of application of the Reynolds Equation for optimization of hydrodynamic bearing conditions.

Example 1: Main Bearing of Internal Combustion Engine

Table 1 Input Parameters

Bearing diameter 68.0 mm 2.6771”
Bearing length 13.0 mm 0.5118”
Rotation speed 2000-7500 RPM 2000-7500 RPM
Force 58831 N 13226 lbs.
Oil inlet temperature 60-100 °C 60-212 °F
Feed pressure 2.0 bar 29.0 psi
Diameter of lubricating hole 3.0 mm 0.12”
Angle of hole position 0 ° 0 °
Width of oil groove 3.0 mm 0.12”
Angle of groove first end 0 ⁰ 0 ⁰
Angle of groove second end 180 ° 180 °
Absolute clearance 5-150 µm 0.2-6.0 thou

Some of the calculation results are presented in Fig.3-6.

fig.3_hydrodynamic_bearing_calculations_and_design.jpg

Fig.3 Effect of Oil Clearance and Rotation Speed on MOFT

The most stable hydrodynamic regime of lubrication is established at the maximum value of minimum oil film thickness (MOFT). According to the graphs in Fig.3, the optimal values of oil clearance for the bearing are as follows:
At 2000 RPM – 50 µm;
At 4000 RPM – 80 µm;
At 7500 RPM – 120 µm.

fig.4_hydrodynamic_bearing_calculations_and_design.jpg

Fig.4 Effect of Oil Clearance and Oil Inlet Temperature on MOFT



Fig.5 Effect of Oil Clearance and Rotation Speed on Power Loss

fig.6_hydrodynamic_bearing_calculations_and_design.jpg

Fig.6 Effect of Oil Clearance and Rotation Speed on Oil Temperature Rise

Example 2: Bushing of Crude Oil Pump

Table 2 Input Parameters

Bearing diameter, mm 35.0 mm 1.3780”
Bearing length 32.0 mm 1.2599”
Rotation speed 50-500 RRM 50-500 RRM
Force 1926 N 433 lbs.
Oil inlet temperature 150 °C 302 °F
Feed pressure 0 bar 0 psi
Absolute clearance 50-100 µm 2.0-4.0 thou

The results of calculations are depicted in Fig.7, 8 Low rotation speeds (100-200 RPM) result in reduction of the values of minimum oil film thickness to the critical level below 0.5 µm (Fig.7).

fig.7_hydrodynamic_bearing_calculations_and_design.jpg

Fig.7 Effect of Rotation Speed and Oil Clearance on MOFT

fig.8_hydrodynamic_bearing_calculations_and_design.jpg

Fig.8 Effect of Oil Clearance and Oil Grade on MOFT

Example 3: Connecting Rod Bearing of Internal Combustion Engine

Table 3 Input Parameters

Bearing diameter 50.0 mm 1.9685”
Bearing length 20.0 mm 0.7874”
Rotation speed 1000-5000 RPM 1000-5000 RPM
Force 50000 N 11240 lbs.
Oil inlet temperature 80 °C 176 °F
Feed pressure 2.5 bar 36 psi
Absolute clearance 10-100 µm 0.4-4.0 thou

The calculations are made for two oil grades having different viscosity. The grade E is more viscous than the Grade D. The results of calculations are depicted in Fig.9-11.

fig.9_hydrodynamic_bearing_calculations_and_design.jpg

Fig.9 Effect of Rotation Speed and Oil Clearance on MOFT for Oil Grades D and E

The graphs in Fig.9 show that the oil grade E produces more stable hydrodynamic lubrication in wide ranges of the oil clearance and rotation speeds. However, the energy losses in hydrodynamic friction with the oil grade E are greater by approx. 60 % than those with the oil grade E (Fig.10).

fig.10_hydrodynamic_bearing_calculations_and_design.jpg

Fig.10 Effect of Rotation Speed and Oil Clearance on Power Loss for Oil Grades D and E

fig.11e_hydrodynamic_bearing_calculations_and_design.jpg
fig.11d_hydrodynamic_bearing_calculations_and_design.jpg

Fig.11 Effect of Rotation Speed and Oil Clearance on Oil Temperature Rise for Oil Grades D and E

Fig.12 depict the effect of the bearing loading on stability of hydrodynamic lubrication within a range of oil clearance value.

fig.12_hydrodynamic_bearing_calculations_and_design.jpg

Fig.12 Effect of Oil Clearance and Bearing Load on MOFT

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Summary

  • Basics of hydrodynamic force are explained by the example of a water skier.
  • Work of hydrodynamic bearing, conditions and principal parameters of hydrodynamic lubrication are considered.
  • Theoretical foundation of hydrodynamic bearing (Reynolds Equation) is described.
  • Practical examples are given on application of Reynolds equation for calculating hydrodynamic conditions of bearing operation: minimum oil film thickness, oil temperature rise, power friction loss.
  • It is shown, how theoretical simulations of hydrodynamic lubrication help to optimize the bearing design and lubrication conditions.


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hydrodynamic_bearing_calculations_and_design.txt · Last modified: 2024/04/30 by dmitri_kopeliovich
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