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Original Articles

Numerical Analyses of Hydrodynamic Lubrication and Dynamics of the Rolling Piston and Crankshaft in a Rotary Compressor

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Pages 1136-1147 | Received 14 Feb 2014, Accepted 30 Jun 2014, Published online: 02 Oct 2014
 

Abstract

In this article, numerical analyses of hydrodynamic lubrication and dynamics of the crank, rolling piston, and vane were carried out to study the tribological performance of a rotary compressor. Dimensionless Reynolds equations of journal and thrust bearings in dynamic load condition were derived and solved numerically. To deal with the lubrication of the rolling piston, the effect of the nonuniformity of tangential velocity over the bearing surface on the Reynolds equation was taken into account. In addition, combined with the analyses of dynamics and kinematics of the crank, piston, and vane, the angular velocities of the crank and piston as well as the motion mode between the piston and vane were studied. Analysis results illustrate characteristic oil film pressure distributions of the crank and piston bearings, which are different from that of common journal bearings. Under the influences of dynamic load and eccentricity of the cam, the wedge effect as well as the stretch and squeeze effect contribute greatly to hydrodynamic pressure. The relative motion mode between the piston and vane tip is not always pure sliding but accompanies rolling in some cases, which depends on the magnitude of the friction coefficient between the piston and vane tip. The analysis results are helpful for the improvement of rotary compressor design.

NOMENCLATURE

c=

Bearing clearance

e=

Eccentricity of the piston and cam, OcOr in Fig. 2

f=

Rated frequency of the motor

Fb=

Pressure force of the oil film of the lower bearing

Fc=

Centrifugal force of the eccentric cam

Fn=

Normal force of the vane top

Fn, Fr=

Reaction force of Fn, Fr

FP=

Force acting on the piston in the compression chamber

FPc, FPs, FP=

Pressure force on the vane ends

FPs=

Force acting on the piston in the suction chamber

Fr=

Friction force in general, either sliding friction force or static friction force

Frp=

Pressure force of the oil film acting on the cam

Frs=

Sliding friction force when it is sliding between the piston and vane

Frt=

Static friction force when it is rolling between the piston and vane

Fs=

Friction force of the oil film at the inner surface of the piston

Fs1=

Friction force of oil film at the surface of the cam

Fsp=

Force of the spring

Fth=

Thrust force of the thrust bearing

Fu=

Pressure force of the oil film of the upper bearing

Fx, Fy=

Pressure force of the oil film acting on the piston

G=

Crank gravity

H=

Dimensionless thickness of the oil film

h=

Thickness of the oil film

hl=

Distance between the center of the lower and upper bearings

Jx, Jy, Jz=

Moment of inertia in the X, Y, and Z directions

L=

Width of bearing, general name of Lb, Lc, and Lu

Lb=

Width of the lower bearing

Lc=

Width of the piston

Lu=

Width of the upper bearing

Lz=

Zb + L/2

Mb=

Friction moment on two side walls of the piston

m=

Mass of the crank

mp=

Mass of the rolling piston

mv=

Mass of the vane

O=

Origin of the coordinate system of XY

Oc=

Circle center of the cam

Or=

Circle center of the piston

=

First- and second-order derivatives of OOr

P=

Dimensionless pressure p

Pc=

Pressure in the compression chamber

Ps=

Pressure in the suction chamber

p=

Pressure of the oil film

p0=

Ambient pressure

R=

Radius of the bearing

r=

Polar radius of the node of the thrust bearing

rb=

Radius of the lower bearing

rc=

Inner radius of the piston

ri=

Inner radius of the thrust bearing

ro=

External radius of the thrust bearing

rp=

External radius of the piston

ru=

Radius of the upper bearing

rv=

Radius of the vane top

Tb, Tu, Trp, Tc, TM=

Moment of Fb, Fu, Frp, Fc, Fth

Tm=

Motor torque

u0=

Tangential velocity on the inner surface of the piston

uh=

Tangential velocity on the surface of the cam

v=

Tangential relative velocity between the piston and vane top

v0=

Normal velocity on the inner surface of the piston

vh=

Normal velocity on the surface of the cam

vr=

Tangential velocity of the piston surface

Wcam=

Work of moment of Frp and Fs1 on the Z axis

WFr=

Work of friction of the upper and lower bearings

WMt=

Work of friction of the thrust bearing

WMz=

Work of moment of Fu and Fb on the Z axis

WTm=

Work of motor torque Tm

xc, yc=

Displacement of the centroid of the crank

=

Second-order derivative of xc, yc

xor, yor=

Displacement of the piston center

=

First- and second-order derivatives of xor, yor

xv=

Displacement of the vane

=

First- and second-order derivatives of xv

Zb=

Coordinate in the axial direction of the bearing, Zb∈[−1/2L,1/2L]

α=

Rotation angle OcOX of the cam in Fig. 2

=

First- and second-order derivatives of α

αt, βt=

Tilt angle of the crank

=

Second-order derivative of αt, βt

β=

Attitude angle of the piston and cam, angle between X and X′ in Fig. 2

γ=

Angle OrAO in Fig. 2

δ=

Thickness of the oil film of the side walls of the piston

ϵ=

Eccentricity ratio of the lower or upper bearings

ϵc=

Eccentricity ratio of the piston and cam, ϵc = e/c

η=

Viscosity of the lubrication oil

θ=

Expanding angle of the bearing

κ=

Angle OrOOv in Fig. 1b

=

First- and second-order derivatives of κ

λ=

Angle between ωc·OOc and u0 in Fig. 2, λ = αβ + θ

μ=

Friction coefficient between the piston and vane top

ρ=

Material density of the piston

τ=

Angle between v0 and the X axis in Fig. 2b

ϕ=

Angle OrOvO in Fig. 1b

=

First- and second-order derivatives of ϕ

ψ=

Attitude angle of the lower or upper bearing

ωc=

Angular velocity of the crank

ωr=

Angular velocity of the piston

=

First-order derivative of ωr

Subscripts

b=

Lower bearing

d=

Dimensionless

u=

Upper bearing

Additional information

Funding

This work was supported by the National Natural Science Foundation of China (NSFC, Grant No. 91123033) and the National Basic Research Program of China (Grant No. 2012CB934101).

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