# Vibration Characteristics of Hydrodynamic Fluid Film Pocket Journal Bearings

Authors: N. S. Feng; E. J. Hahn
Journal: Advances in Acoustics and Vibration
 (2010)

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## Abstract

Theoretical analyses of hydrodynamic fluid film bearings with different bearing profiles rely on solutions of the Reynolds equation. This paper presents an approach used for analysing the so-called pocket bearings formed from a combination of offset circular bearing profiles. The results show that the variation of the dynamic bearing characteristics with different load inclinations for the pocket bearings is less than that for the elliptic bearing counterpart. It is shown that the natural frequencies as well as the critical speeds, and hence the vibrational behaviour, can also be significantly different for an industrial rotor supported by the different bearings.


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## Body

## 1. Introduction

In order to increase productivity and reduce machine downtime, hydrodynamic bearings are frequently used to support high-speed rotating machinery where reliability, long running life, and minimum vibration levels are of primary concern. Simple circular bore journal bearings sometimes cause instability, which may result in catastrophic failure of the machinery. To improve resistance to such failure, different bearing types with different bearing clearance profiles have been developed and used in practice. Typical examples are elliptic bearings and tilting pad bearings, the former providing stabilizing preload and the latter minimizing the troublesome cross-coupled bearing forces. Another bearing type, formed by a combination of offset circular bearing profiles and referred to as a pocket bearing, is also sometimes used in machinery such as turbogenerators.The theoretical analysis of hydrodynamic bearings relies on the solutions of Reynolds equation, a partial differential equation derived from the Navier-Stokes and continuity equations under certain simplifying assumptions [1]. In order to minimise the computational effort, particularly in transient response analyses, some further simplifications such as infinitely short or long bearing approximations are frequently used [2]. Improvements to these techniques to achieve better solution accuracy using more complicated yet still manageable approaches have also been developed [3]. Alternatively, for steady-state solutions where it is possible to prepare the bearing data a priori, numerical solutions to the full Reynolds equation can be tabulated or plotted for subsequent use [4]. For different bearing types, the different bearing clearance profiles need to be considered when obtaining the corresponding solutions [5]. Such data is also needed for the different types of pocket bearings, whose respective static and dynamic characteristics are of interest. This paper illustrates the approach used to obtain solutions for these pocket bearings.


## 2. Theory

### 2.1. General Theory

The schematic of a simple circular hydrodynamic fluid film bearing is shown in Figure1. Following the usual assumptions of hydrodynamic lubrication theory, the Reynolds equation can be written as [1](1)∂∂X(h3∂P∂X)+∂∂Z(h3∂P∂Z)=-6μU∂h∂X+12μV,
where
(2)h=C-zsinψ-ycos⁡ψ,(3)ψ=θ+ϕ+π2.
Upon nondimensionalisation, (1) becomes
(4)∂∂ψ(h¯3∂P¯∂ψ)+(DL)2∂∂Z¯(h¯3∂P¯∂Z¯)=-[(2z¯′-y¯)sinψ+(2y¯′+z¯)cos⁡ψ],
in which(5)Z¯=ZL/2,P¯=P6μω(R/C)2,h¯=hC=1-z¯sinψ-y¯cos⁡ψ,y¯=yC,and so forth.h¯′=-z¯′sinψ-y¯′cos⁡ψ.
The pressure boundary conditions are that P¯=0 at Z¯=±1 (bearing edges) and at ψ1 and ψ2 (the boundary coordinates at the onset and end of the fluid film, resp.). The Reynolds cavitation boundary condition is used to define the cavitation region [1].Figure 1
Schematic of a circular bearing.Upon integration of the film pressure, the fluid film force components iny and z directions are
(6)(FyFz)=-∫ψ1ψ2∫-L/2L/2P(cos⁡ψsinψ)RdZdψ=(0W).
The corresponding nondimensional force components are [3](7)(fyfz)=-3∫ψ1ψ2∫-11P¯(cos⁡ψsinψ)dZ¯dψ=(01πS).
For small perturbations Δy̅, Δz̅, Δy̅′, and Δz̅′ in the y and z directions about the equilibrium position, the dynamic bearing coefficients are defined as
(8)(ΔfzΔfy)=-[KzzKzyKyzKyy](Δz̅Δy̅)-[CzzCzyCyzCyy](Δz̅′Δy̅′).
Ignoring higher-order terms, the Taylor series expansion about the equilibrium position (y̅o, z̅o, y̅′=0 and z̅′=0) yields Kzz=-∂fz/∂z̅,Czy=-∂fz/∂y̅′, and so forth.Note that for more than one pad or clearance profile, it is the resultant of the forces on all the pads or clearance profiles in they and z directions which equals zero and W, respectively, in (6); it is the perturbation in these resultant force components which is used to evaluate the dynamic bearing coefficients.The above is the summary of the general theory for determining the static and dynamic bearing characteristics (i.e., Sommerfeld number, attitude angle, stiffness coefficients, and damping coefficients). Different bearing configurations impose different geometric relationships for the position of the journal in the bearing.


### 2.2. Pocket Bearing Configurations

Two types of pocket bearings are to be considered. The first type, formed in a similar way to an elliptic bearing (Figure2), is schematically shown in Figure 3 and is referred to as type 1. The two halves of a bearing block are held together, separated by shims corresponding to the ellipticity 2d1. A circular hole of diameter D is cut, and the shims are then removed to form a normal elliptic bearing with the top pad centre a distance d1 below, and the bottom pad centre a distance d1 above the bearing centre. Concentric arc portions (the pockets) of a specified angular extent are then machined as shown in Figure 3. Such a pocket bearing has three curvature centres: one above one below the bearing centre for the side arcs just like the elliptic bearings and one coinciding with the bearing centre for the pockets.Figure 2
Schematic of an elliptic bearing.Figure 3
Schematic of type-1 pocket bearing.The second type of pocket bearing, referred to as type 2, is shown schematically in Figure4. It can be conveniently machined by NC machines. It also has three arc centres, but the two for the side arcs are located at a distance d2 to the left and right of the bearing centre, the left centre for the left arcs on both the top and bottom pads, and the right one for the right arcs, again on both pads. The angular extent of the side arcs is determined by the arc radii and the centre offset d2. The two types of the pocket bearings are expected to have similar vibration characteristics.Figure 4
Schematic of type-2 pocket bearing.Normally, the bearing clearanceC is used to nondimensionalise the film thickness and the relative journal to bearing displacements. Due to the bearing profile, each pocket bearing has two clearances: Cp for the pocket portion and Ce for the side arcs. Using different clearances will produce different nondimensional bearing coefficients, but for a given bearing, the dimensional coefficients should not be affected. Following the approach for elliptic bearings [5], Ce could be chosen as the nondimensionalising parameter. However, the type-2 pocket bearing does not have such a corresponding clearance, though it also has two clearances: Cp for the pocket portion and Cs for the side arcs. Hence, in order to have comparable results, the pocket clearance Cp, common to both types of pocket bearings, is used as the nondimensionalising parameter.


### 2.3. Type-One Pocket Bearing

From (2), the nondimensional film thickness for the side arcs becomes
(9)h¯e=CeCp-z¯sinψ-y¯cos⁡ψ
and for the pocket arcs
(10)h¯p=1-z¯sinψ-y¯cos⁡ψ.
Note that in these equations, y¯ and z¯ are the nondimensional journal centre coordinates from the corresponding arc centres.For the pocket portion:(11)y¯p=εsin(ϕ-β),z¯p=-εcos⁡(ϕ-β),
and for the bottom side arcs,(12)y¯b=εbsin(ϕb-β),z¯b=-εbcos⁡(ϕb-β),
where, from Figure 5,(13)εb=ε2+δ2+2εδcos⁡ϕ,sinϕb=εεbsin(180°-ϕ).
For the top side arcs,(14)y¯t=εtsin(ϕt-β),z¯t=-εtcos⁡(ϕt-β),
where, from Figure 5,(15)εt=ε2+δ2-2εδcos⁡ϕ,sin(180°-ϕt)=εεtsinϕ.
The clearances Ce and Cp are related by the pocket arc extent α and the ellipticity of the side arcs d1. As shown in Figure 6, at the intersection between the side and pocket arcs, one has
(16)Re2=Rp2+d12-2Rpd1cos⁡(180°-α2).
Solving for Rp and omitting higher-order terms(17)Rp=-d1cos⁡(α2)+Re2-d12sin2(α2)≈Re-d1cos⁡(α2).
The journal radius can be expressed as
(18)r=Re-Ce=Rp-Cp.
Substitution of (17) into (18) gives(19)Ce-Cp=Re-Rp≈d1cos⁡(α2),
or
(20)CeCp≈1+d1cos⁡(α/2)Cp=1+δ1cos⁡(α2)
which is always greater than 1.Figure 5
Geometric relationship between the arc centres for elliptic and type-1 pocket bearings.Figure 6
Geometric relationship betweenCe and Cp for type-1 pocket bearing.


### 2.4. Type-Two Pocket Bearing

Again, following an approach similar to that for the type 1 bearings, one has for the side arcs(21)h¯s=CsCp-z¯sinψ-y¯cos⁡ψ
and for the pocket arcs(22)h¯p=1-z¯sinψ-y¯cos⁡ψ.
The clearances Cs and Cp are related by the pocket arc extent α and the offset of the side arc centers d2.As shown in Figure 7, at the intersection between the side and pocket arcs, one has
(23)Rs2=Rp2+d22-2Rpd2cos⁡(90∘-α2).
Solving for Rp and omitting higher-order terms,
(24)Rp=d2sin(α2)+Rs2-d22cos⁡2(α2)≈Rs+d2sin(α2).
The journal radius can be expressed as
(25)r=Rs-Cs=Rp-Cp.
From (24) and (25), this gives(26)Cp-Cs≈d2sin(α2),
or
(27)CsCp≈1-d2sin(α/2)Cp=1-δ2sin(α2).
To relate the offset d2 to the ellipticity d1, it is assumed that, apart from the same pocket arc extent α, the horizontal widths of the two bearings are the same, that is,
(28)Rs+d2=Re2-d12≈Re.
Substitution of (24) and (17) into (28) gives(29)Rp-d2sin(α2)+d2=Rp+d1cos⁡(α2),
or(30)d2=d1cos⁡(α/2)1-sin(α/2).Figure 7
Geometric relationship betweenCs and Cp for type-2 pocket bearings.The relationships betweeny¯, z¯ and ε, ϕ are the same as before. However, the calculations for εl, εr, ϕl, and ϕr need different expressions. From Figure 8,
(31)εl=ε2+δ22+2εδ2sinϕ,sin(90°-ϕl)=εεlsin(90°+ϕ),εr=ε2+δ22-2εδ2sinϕ,sin(90°+ϕr)=εεrsin(90°-ϕ).Figure 8
Geometric relationship between the arc centres for type-2 pocket bearing.


## 2.1. General Theory

The schematic of a simple circular hydrodynamic fluid film bearing is shown in Figure1. Following the usual assumptions of hydrodynamic lubrication theory, the Reynolds equation can be written as [1](1)∂∂X(h3∂P∂X)+∂∂Z(h3∂P∂Z)=-6μU∂h∂X+12μV,
where
(2)h=C-zsinψ-ycos⁡ψ,(3)ψ=θ+ϕ+π2.
Upon nondimensionalisation, (1) becomes
(4)∂∂ψ(h¯3∂P¯∂ψ)+(DL)2∂∂Z¯(h¯3∂P¯∂Z¯)=-[(2z¯′-y¯)sinψ+(2y¯′+z¯)cos⁡ψ],
in which(5)Z¯=ZL/2,P¯=P6μω(R/C)2,h¯=hC=1-z¯sinψ-y¯cos⁡ψ,y¯=yC,and so forth.h¯′=-z¯′sinψ-y¯′cos⁡ψ.
The pressure boundary conditions are that P¯=0 at Z¯=±1 (bearing edges) and at ψ1 and ψ2 (the boundary coordinates at the onset and end of the fluid film, resp.). The Reynolds cavitation boundary condition is used to define the cavitation region [1].Figure 1
Schematic of a circular bearing.Upon integration of the film pressure, the fluid film force components iny and z directions are
(6)(FyFz)=-∫ψ1ψ2∫-L/2L/2P(cos⁡ψsinψ)RdZdψ=(0W).
The corresponding nondimensional force components are [3](7)(fyfz)=-3∫ψ1ψ2∫-11P¯(cos⁡ψsinψ)dZ¯dψ=(01πS).
For small perturbations Δy̅, Δz̅, Δy̅′, and Δz̅′ in the y and z directions about the equilibrium position, the dynamic bearing coefficients are defined as
(8)(ΔfzΔfy)=-[KzzKzyKyzKyy](Δz̅Δy̅)-[CzzCzyCyzCyy](Δz̅′Δy̅′).
Ignoring higher-order terms, the Taylor series expansion about the equilibrium position (y̅o, z̅o, y̅′=0 and z̅′=0) yields Kzz=-∂fz/∂z̅,Czy=-∂fz/∂y̅′, and so forth.Note that for more than one pad or clearance profile, it is the resultant of the forces on all the pads or clearance profiles in they and z directions which equals zero and W, respectively, in (6); it is the perturbation in these resultant force components which is used to evaluate the dynamic bearing coefficients.The above is the summary of the general theory for determining the static and dynamic bearing characteristics (i.e., Sommerfeld number, attitude angle, stiffness coefficients, and damping coefficients). Different bearing configurations impose different geometric relationships for the position of the journal in the bearing.


## 2.2. Pocket Bearing Configurations

Two types of pocket bearings are to be considered. The first type, formed in a similar way to an elliptic bearing (Figure2), is schematically shown in Figure 3 and is referred to as type 1. The two halves of a bearing block are held together, separated by shims corresponding to the ellipticity 2d1. A circular hole of diameter D is cut, and the shims are then removed to form a normal elliptic bearing with the top pad centre a distance d1 below, and the bottom pad centre a distance d1 above the bearing centre. Concentric arc portions (the pockets) of a specified angular extent are then machined as shown in Figure 3. Such a pocket bearing has three curvature centres: one above one below the bearing centre for the side arcs just like the elliptic bearings and one coinciding with the bearing centre for the pockets.Figure 2
Schematic of an elliptic bearing.Figure 3
Schematic of type-1 pocket bearing.The second type of pocket bearing, referred to as type 2, is shown schematically in Figure4. It can be conveniently machined by NC machines. It also has three arc centres, but the two for the side arcs are located at a distance d2 to the left and right of the bearing centre, the left centre for the left arcs on both the top and bottom pads, and the right one for the right arcs, again on both pads. The angular extent of the side arcs is determined by the arc radii and the centre offset d2. The two types of the pocket bearings are expected to have similar vibration characteristics.Figure 4
Schematic of type-2 pocket bearing.Normally, the bearing clearanceC is used to nondimensionalise the film thickness and the relative journal to bearing displacements. Due to the bearing profile, each pocket bearing has two clearances: Cp for the pocket portion and Ce for the side arcs. Using different clearances will produce different nondimensional bearing coefficients, but for a given bearing, the dimensional coefficients should not be affected. Following the approach for elliptic bearings [5], Ce could be chosen as the nondimensionalising parameter. However, the type-2 pocket bearing does not have such a corresponding clearance, though it also has two clearances: Cp for the pocket portion and Cs for the side arcs. Hence, in order to have comparable results, the pocket clearance Cp, common to both types of pocket bearings, is used as the nondimensionalising parameter.


## 2.3. Type-One Pocket Bearing

From (2), the nondimensional film thickness for the side arcs becomes
(9)h¯e=CeCp-z¯sinψ-y¯cos⁡ψ
and for the pocket arcs
(10)h¯p=1-z¯sinψ-y¯cos⁡ψ.
Note that in these equations, y¯ and z¯ are the nondimensional journal centre coordinates from the corresponding arc centres.For the pocket portion:(11)y¯p=εsin(ϕ-β),z¯p=-εcos⁡(ϕ-β),
and for the bottom side arcs,(12)y¯b=εbsin(ϕb-β),z¯b=-εbcos⁡(ϕb-β),
where, from Figure 5,(13)εb=ε2+δ2+2εδcos⁡ϕ,sinϕb=εεbsin(180°-ϕ).
For the top side arcs,(14)y¯t=εtsin(ϕt-β),z¯t=-εtcos⁡(ϕt-β),
where, from Figure 5,(15)εt=ε2+δ2-2εδcos⁡ϕ,sin(180°-ϕt)=εεtsinϕ.
The clearances Ce and Cp are related by the pocket arc extent α and the ellipticity of the side arcs d1. As shown in Figure 6, at the intersection between the side and pocket arcs, one has
(16)Re2=Rp2+d12-2Rpd1cos⁡(180°-α2).
Solving for Rp and omitting higher-order terms(17)Rp=-d1cos⁡(α2)+Re2-d12sin2(α2)≈Re-d1cos⁡(α2).
The journal radius can be expressed as
(18)r=Re-Ce=Rp-Cp.
Substitution of (17) into (18) gives(19)Ce-Cp=Re-Rp≈d1cos⁡(α2),
or
(20)CeCp≈1+d1cos⁡(α/2)Cp=1+δ1cos⁡(α2)
which is always greater than 1.Figure 5
Geometric relationship between the arc centres for elliptic and type-1 pocket bearings.Figure 6
Geometric relationship betweenCe and Cp for type-1 pocket bearing.


## 2.4. Type-Two Pocket Bearing

Again, following an approach similar to that for the type 1 bearings, one has for the side arcs(21)h¯s=CsCp-z¯sinψ-y¯cos⁡ψ
and for the pocket arcs(22)h¯p=1-z¯sinψ-y¯cos⁡ψ.
The clearances Cs and Cp are related by the pocket arc extent α and the offset of the side arc centers d2.As shown in Figure 7, at the intersection between the side and pocket arcs, one has
(23)Rs2=Rp2+d22-2Rpd2cos⁡(90∘-α2).
Solving for Rp and omitting higher-order terms,
(24)Rp=d2sin(α2)+Rs2-d22cos⁡2(α2)≈Rs+d2sin(α2).
The journal radius can be expressed as
(25)r=Rs-Cs=Rp-Cp.
From (24) and (25), this gives(26)Cp-Cs≈d2sin(α2),
or
(27)CsCp≈1-d2sin(α/2)Cp=1-δ2sin(α2).
To relate the offset d2 to the ellipticity d1, it is assumed that, apart from the same pocket arc extent α, the horizontal widths of the two bearings are the same, that is,
(28)Rs+d2=Re2-d12≈Re.
Substitution of (24) and (17) into (28) gives(29)Rp-d2sin(α2)+d2=Rp+d1cos⁡(α2),
or(30)d2=d1cos⁡(α/2)1-sin(α/2).Figure 7
Geometric relationship betweenCs and Cp for type-2 pocket bearings.The relationships betweeny¯, z¯ and ε, ϕ are the same as before. However, the calculations for εl, εr, ϕl, and ϕr need different expressions. From Figure 8,
(31)εl=ε2+δ22+2εδ2sinϕ,sin(90°-ϕl)=εεlsin(90°+ϕ),εr=ε2+δ22-2εδ2sinϕ,sin(90°+ϕr)=εεrsin(90°-ϕ).Figure 8
Geometric relationship between the arc centres for type-2 pocket bearing.


## 3. Solution Procedures

To calculate the static and dynamic characteristics of the pocket bearings, Gauss-Seidel iteration with successive over relaxation is used to solve the finite difference formulation of the Reynolds equation [5], thereby ensuring that the Reynolds condition is used as the cavitation boundary. All results here assume same zero gauge inlet, outlet, and cavitation pressures.


## 4. Results

Figure9 compares the nondimensional static and dynamic characteristics of the two types of pocket bearings as a function of load inclination beta (β), using the same base clearance Cp and the the same pocket extent of α=60°. Apart from some difference in the attitude angle, the nondimensional characteristics are virtually identical.Comparison of the nondimensional bearing characteristics for the two types of pocket bearings ((1) and (2) correspond to type 1 and 2, resp.).
(a)(b)(c)Figures10 and 11 compare the bearing characteristics of the type-1 pocket bearing to a similar elliptic bearing as functions of the load inclination angle β for given eccentricities ε=0.2 and 0.4, respectively. It can be seen that in general there is less variation in the dynamic bearing characteristics of the pocket bearing due to the change of β.Nondimensional bearing characteristics for elliptic and type-1 pocket bearings atε=0.2.
(a)(b)(c)(d)(e)(f)Nondimensional bearing characteristics for elliptic and type-1 pocket bearings atε=0.4.
(a)(b)(c)(d)(e)(f)A sample vibration analysis is also performed for an industrial rotor subjected to gravity loading and supported on either type of pocket bearings or similar elliptic bearings. The rotor is shown schematically in Figure12. Table 1 lists the corresponding data used to characterise the rotor and the bearings. In house vibration analysis software was used to determine the natural frequencies and mode shapes over a speed range up to 5000 rpm. Table 2 lists these natural frequencies, and Figure 13 shows the Campbell diagrams for the elliptic bearing supports and for the type-1 pocket bearing supports.Table 1
Sample rotor bearing data.
Rotor: Young’s modulus = 210 GPa, density = 7850 kg/m3No.Length (m)Diameter (m)Disk mass (kg)Disk Ip (kg-m2)Disk Id (kg-m2)10.140.13500.03580.043620.160.1800.12940.132930.1480.1800.11930.113140.1480.1800.11930.113150.1150.2588.3920.54470.333660.1150.2771.1850.54470.333670.1150.2771.1850.54470.333680.1060.32811.871.2910.721790.1060.3530.9211.2910.7217100.0490.34500.5350.2747110.0760.4489.298.6434.408120.0580.547.736.5593.317130.150.55693.8620.578.875140.2240.556139.530.4814.42150.20.55611125.3812.52160.2190.556128.428.5714170.2170.556126.628.1913.88180.2160.556122.827.5713.77190.2150.556119.127.0513.66200.2140.556119.126.8713.59210.2210.547126.726.8313.6220.1980.55117.224.6412.55230.1590.7044.1530.6216.34240.1590.7044.1530.6216.34250.160.497249.430.8116.46260.0150.34500.16380.0821270.1680.3531.4672.0561.335280.1680.3531.4672.0561.335290.170.3531.4842.0811.359300.1870.31501.4191.043310.070.38538.393.0341.559320.2380.31501.8061.59330.2380.31501.8061.59340.0670.4225.12.9041.489350.0650.5867.2112.736.436360.070.5813122.111.16Bearings:δ=0.5, (α=60° for pocket bearings)No.Length (m)Diameter (m)Clearance (mm)Viscosity (Ns/m2)Location10.0920.180.13270.014220.2040.3150.23220.01432Table 2
Damped natural frequencies of a rotor supported by elliptic or pocket bearings ((1) refers to type 1, etc.).
Speed (rpm)10002000300040005000EllipticReal, Imag (rad/s)Mode 1-19.91,137.5-11.17,143.9-7.588,150.4-5.047,156.1-3.323,160.8Mode 2-4.064,211.8-5.900,207.7-6.266,204.2-5.913,201.6-5.291,199.6Mode 3-129.3,217.4-89.73,261.5-84.35,288.3-79.77,317.3-70.84,344.6PocketReal, Imag (rad/s)Mode 1(1)-27.05,192.6-19.47,183.2-10.63,184.8-5.012,189.2-1.620,193.4(2)-30.75,186.0-23.41,175.1-15.76,177.6-9.796,182.3-6.021,186.6Mode 2(1)-3.379,212.6-4.965,209.7-5.133,207.6-4.768,206.3-4.255,205.4(2)-3.633,212.0-4.647,208.7-4.249,206.8-3.419,205.9-2.527,205.6Mode 3(1)-162.5,75.30-246.2,140.1-300.0,189.1-352.9,237.0-418.2,293.1(2)-201.1,48.79-331.0,79.78-390.9,114.1-473.7,166.2-566.0,241.0Mode 4(1)-85.34,57.67-140.8,121.7-194.9,206.5-223.7,315.3-202.6,425.3(2)-111.7,29.36-196.7,118.1-258.1,265.9-212.5,394.2-155.1,462.0Figure 12
Sample rotor bearing system.Campbell diagrams for a rotor supported by (a) elliptic bearings or (b) type-1 pocket bearings.
(a)(b)It can be seen that the system behaves quite differently with the different types of bearing supports. The rotor with the elliptic bearing has three natural frequencies but two critical speeds in the speed range; while the rotor with the type-1 pocket bearing has four natural frequencies but only one critical speed. The second mode in both cases is a backward whirl and is therefore unlikely to be excited. Using equivalent clearances for the different pocket bearing models, the natural frequencies in Table2 indicate that the two types of the pocket bearings with similar dimensions could have quite different effects on the system vibration characteristics.


## 5. Conclusions

An approach to evaluate the static and dynamic bearing characteristics of pocket type bearings, suited for subsequent steady-state vibration analysis of rotating machinery involving such bearings, is presented.Compared to similar elliptic bearings, the pocket bearings tend to provide less fluctuation in the dynamic bearing coefficients for different load inclinations and may produce significantly different vibration behaviour in a given rotor system.The two types of pocket bearings investigated here (produced by different machining procedures), apart from some difference in attitude angle, have virtually identical static and dynamic bearing characteristics



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