Experimental Characterization of Large Turbomachinery Tilting Pad Journal Bearings

: The paper deals with the experimental characterization of different 280 mm diameter tilting pad journal bearings for turbomachines using a dedicated test rig. The test articles were a 5-pad Direct Lube Rocker Pivot bearing, a 5-pad Flooded Rocker Pivot bearing, and a 4-pad Flooded Ball and Socket Pivot bearing. The three bearings were tested in their speciﬁc design range of operating conditions. Their static and dynamic behavior was investigated as a function of different operating parameters. In particular, the assumed journal center eccentricity and pads temperature were measured, and the power loss determined as a function of angular speed for different static loads. Dynamic stiffness and damping coefﬁcients were determined as a function of excitation frequency for different speeds and loads. The experimental results were compared showing the inﬂuence of the operating parameters, conﬁguration, and oil supply.


Introduction
Tilting pad journal bearings (TPJB) are essential components for supporting the rotors of turbomachinery industrial applications, guaranteeing stability and efficiency even in increasingly severe operating conditions in terms of load and speed.
TPJBs have been the subject of extensive theoretical and experimental studies in recent decades focusing in particular on their dynamic characteristics. For reviews, refer to [1,2]. However, many aspects still need to be clarified to increase the reliability of numerical simulation and prediction tools, particularly useful at the design stage. Therefore, it is necessary to carry out test campaigns, extending the fields of exploration in terms of bearing size, geometric configuration, oil supply, and operating conditions. The "component level" test approach is generally used in new product development programs in order to reduce the risk associated to the adoption of new design components.
A certain number of test rigs have been set up in the labs all over the world differing in size, range of operating conditions, and configuration. Most of them adopt the floating bearing configuration where loads are applied to the bearing and the rotor bearing relative displacement is measured, as, for example, in [3][4][5][6][7][8], while a few adopt the floating rotor configuration where the loads are applied to the rotor instead [9]. Identification methods, mainly in the frequency domain as proposed in [3], allow one to determine the dynamic coefficients. Effects on bearing behaviour of load direction [10], pivot stiffness [11] and flexural pivot [12], nonlinearities [13] have been evaluated.
As regards the effect of size, quite large size bearings working at high peripheral speeds have been tested and characterized both statically and dynamically in a few labs. Bearings of 500 mm nominal diameter have been tested on a test rig which provides high  The rotor of the test bearing is connected to a single stage gear multiplier with the low-speed shaft connected to a 630 kW electric motor controlled by an inverter. A torque meter with 1 kNm full scale is located between the test section and the gearbox with a gear ratio 6:1. The motor maximum speed is 4000 rpm so that the theoretical rotor maximum rotational speed is 24,000 rpm. The nominal torque of the motor is 3000 Nm. The experimental apparatus is used to perform both static and dynamic tests employing hydraulic actuators. Their full scales are 270 kN for the static load actuator and 30 kN for the dynamic ones. Dynamic loads can be applied at frequencies up to 350 Hz. Three independent oil systems are used for supplying the lubricant to the tested bearing, to the hydraulic actuators, and to the gearbox. The main characteristics of the lubrication systems are reported in Table 1, that summarize the capabilities of the experimental plant. Due to the high power dissipated oil-water heat exchangers and 700 kW cooling towers are employed. A complex control and data acquisition system is used able to record about 30 high-frequency signals (up to 100 kHz) and 60 low-frequency signals normally sampled   The rotor of the test bearing is connected to a single stage gear multiplier with the low-speed shaft connected to a 630 kW electric motor controlled by an inverter. A torque meter with 1 kNm full scale is located between the test section and the gearbox with a gear ratio 6:1. The motor maximum speed is 4000 rpm so that the theoretical rotor maximum rotational speed is 24,000 rpm. The nominal torque of the motor is 3000 Nm. The experimental apparatus is used to perform both static and dynamic tests employing hydraulic actuators. Their full scales are 270 kN for the static load actuator and 30 kN for the dynamic ones. Dynamic loads can be applied at frequencies up to 350 Hz. Three independent oil systems are used for supplying the lubricant to the tested bearing, to the hydraulic actuators, and to the gearbox. The main characteristics of the lubrication systems are reported in Table 1, that summarize the capabilities of the experimental plant. Due to the high power dissipated oil-water heat exchangers and 700 kW cooling towers are employed. A complex control and data acquisition system is used able to record about 30 high-frequency signals (up to 100 kHz) and 60 low-frequency signals normally sampled

Test Section and Test Types
A configuration with floating bearing housing and fixed axis rotor is used for the test section ( Figure 3). In this configuration, the static and dynamic loads are applied to the bearing housing and the rotor is supported by two rolling bearings. The bearing housing consists of two semi-housings, a lower and an upper one, positioned through two pins with a design clearance and fixed by bolts.

Test Section and Test Types
A configuration with floating bearing housing and fixed axis rotor is used for the test section ( Figure 3). In this configuration, the static and dynamic loads are applied to the bearing housing and the rotor is supported by two rolling bearings. The bearing housing consists of two semi-housings, a lower and an upper one, positioned through two pins with a design clearance and fixed by bolts. The static load is applied upwards in the vertical direction, while the dynamic load is obtained by using two identical hydraulic actuators controlled in force. They are positioned at 45° with respect to the vertical direction, so that they are mutually orthogonal, and can work one at a time or simultaneously. The pistons of the dynamic jacks are supported by hydrostatic bearings in order to limit friction. Instrumented stingers that have high longitudinal stiffness and small transverse ones are interposed between the actuators and the bearing housing. An axial load cell between the actuator and the stinger is used to measure the static load. The stingers of the dynamic actuators are triaxial load cells that The static load is applied upwards in the vertical direction, while the dynamic load is obtained by using two identical hydraulic actuators controlled in force. They are positioned at 45 • with respect to the vertical direction, so that they are mutually orthogonal, and can work one at a time or simultaneously. The pistons of the dynamic jacks are supported by hydrostatic bearings in order to limit friction. Instrumented stingers that have high longitudinal stiffness and small transverse ones are interposed between the actuators and the bearing housing. An axial load cell between the actuator and the stinger is used to measure the static load. The stingers of the dynamic actuators are triaxial load cells that also measure all tangential force components. An anti-roll arm is used to reduce the tangential forces on the stingers by limiting the rotation of the housing due to the bearing friction torque. An axial load cell is placed between the anti-roll arm and the basement.
It is noteworthy that the force constraints due to the interactions of the three actuators are minimized by means of the flexible stingers. Nonetheless, in spite of the unavoidable residual interactions of the actuators, since the bearing housing is constrained transversally only by load cells, all the transversal loads applied to the bearing are measured and can be used as force input together with the bearing displacement in the 2D dynamic model identification algorithm to determine the bearing dynamic characteristics.
Three pitch stabilizers (anti-pitch rod), at 120 • around the bearing provide axial constraints (negligible transversal constraint) to the bearing housing ( Figure 4). They are also used to align the bearing with respect to the rotor, through an iterative procedure, acting on two opposite bolts placed on their threaded central bodies.
sally only by load cells, all the transversal loads applied to the bearing are measured and can be used as force input together with the bearing displacement in the 2D dynamic model identification algorithm to determine the bearing dynamic characteristics.
Three pitch stabilizers (anti-pitch rod), at 120° around the bearing provide axial constraints (negligible transversal constraint) to the bearing housing ( Figure 4). They are also used to align the bearing with respect to the rotor, through an iterative procedure, acting on two opposite bolts placed on their threaded central bodies. Eight high-resolution proximity sensors are used to measure the radial relative displacements between the bearing housing and the rotor on two parallel planes perpendicular to the bearing axis. Four accelerometers measure the acceleration of the bearing housing at the mid-section ( Figure 3). More information about all the sensors used for the dynamic characterization of the bearing is given in Table 2. The test section was primarily designed to test large size TPJBs with diameters from 150 to 300 mm, axial length to diameter ratio L/D = 0.4-1.0, and peripheral speeds up to 150 m/s. Bearings with diameters from 250 to 300 mm can be tested with minor modifica- Eight high-resolution proximity sensors are used to measure the radial relative displacements between the bearing housing and the rotor on two parallel planes perpendicular to the bearing axis. Four accelerometers measure the acceleration of the bearing housing at the mid-section ( Figure 3). More information about all the sensors used for the dynamic characterization of the bearing is given in Table 2. The test section was primarily designed to test large size TPJBs with diameters from 150 to 300 mm, axial length to diameter ratio L/D = 0.4-1.0, and peripheral speeds up to 150 m/s. Bearings with diameters from 250 to 300 mm can be tested with minor modifications, essentially using a shaft with suitable diameter. Some major modifications are instead necessary for testing bearings with lower diameters due to the different range of stiffness involved, leading to lower shaft frequencies.
Static and dynamic tests can be performed. A bump test is also usually carried out to identify the bearing clearance, center, and alignment by applying a low frequency rotating force generated by two sinusoidal forces with 90 • phase shift, produced by the dynamic actuators. Low-frequency signals are recorded under stationary conditions at different load, speed, oil temperature, and flow rate. Typical collected data are forces, torque, displacements, rotational speed, temperatures, pressures, flow rates in the main and auxiliary lubrication systems.
The dynamic tests are performed to identify the bearing stiffness and damping coefficients. Sinusoidal forces at the desired frequency and amplitude are produced by the dynamic actuators. A vertical force is produced with the actuators operating in phase with equal amplitude and frequency and a horizontal force when operating in antiphase. The main high frequency collected data are forces, displacements, and accelerations. Some characteristics of the experimental rig with the present test section for bearings with 280 mm inner diameter are reported in Table 3.

Dynamic Coefficients Identification Method
To avoid imbalance disturbance, synchronous values of the dynamic coefficients are not directly obtained by testing at the rotational frequency but by an interpolation of the results obtained at different frequencies chosen below and above the rotational frequency. In order to decrease the acquisition time, the forces applied during excitation can contain more frequency components ("multitone" test) instead of a single frequency ("single tone" test). Two linearly independent tests are necessary for the identification of the dynamic coefficients for each working condition. Usually, tests with vertical and horizontal dynamic forces are performed with amplitudes of each sinusoidal load tuned in order to have a displacement amplitude sufficiently high for the analysis but not so high to produce nonlinear behaviors [13]. Signals of force, displacement, and acceleration are then processed in the frequency domain using the Fast Fourier Transform (FFT), separating the different frequency components. The bearing film force is firstly determined by subtracting the bearing housing inertia from the measured forces acting on the housing: where F indicates the amplitude of the force FFT, A the amplitude of the acceleration FFT, M the housing mass; the subscripts b and h refer to bearing and housing, x and y refer to the horizontal and vertical direction, a and i to the anti-phase and in-phase test, respectively. The stiffness and damping coefficients are obtained as the real and imaginary parts of the bearing impedance matrix determined in the frequency domain by multiplying the [ where H indicates the complex elements of the impedance matrix, k and c the stiffness and damping coefficients, respectively, and D the amplitude of the displacement.

Tested Bearings
Three TPJBs were tested: the Direct Lube Rocker Pivot bearing, the Flooded Rocker Pivot bearing, and the Flooded Ball & Socket Pivot bearing. The bearings are shown in Figure 5 and their characteristics are summarized in Table 4. According to Baker Hughes nomenclature, bearing lubrication layouts are classified as: • flooded lubrication when the end seals clearance is low enough to get pressurized bearing housings; • direct lubrication when all the required oil is supplied by oil inlet orifices/spray bars and the bearing cavity is evacuated through the adoption of larger end seals clearance with respect to flooded configurations.
damping coefficients, respectively, and D the amplitude of the displacement.

Tested Bearings
Three TPJBs were tested: the Direct Lube Rocker Pivot bearing, the Flooded Rocker Pivot bearing, and the Flooded Ball & Socket Pivot bearing. The bearings are shown in Figure 5 and their characteristics are summarized in Table 4. According to Baker Hughes nomenclature, bearing lubrication layouts are classified as: • flooded lubrication when the end seals clearance is low enough to get pressurized bearing housings; • direct lubrication when all the required oil is supplied by oil inlet orifices/spray bars and the bearing cavity is evacuated through the adoption of larger end seals clearance with respect to flooded configurations.
(a) (b) (c)  The scheme of the pivot geometry is shown in Figure 6 for the Load-between-Pivot configuration. The 5-pad configuration is shown on the left and the 4-pad on the right.  The scheme of the pivot geometry is shown in Figure 6 for the Load-between-Pivot configuration. The 5-pad configuration is shown on the left and the 4-pad on the right.
In the following schemes, the direction of the shaft rotation is indicated as seen from the side opposite to the driver side.
The Direct Lube Rocker Pivot bearing ( Figure 5a) is a high-speed 5-pad TPJB that was designed with the aim of reaching high peripheral speeds (>100 m/s). The pads are connected to the bearing housing by means of a cylindrical pivot ( Figure 6). The pad arc geometry and the particular scheme of the lubrication layout were defined through an optimization process to target the required static and dynamic performance in the entire speed range. Each pad is instrumented with two thermocouples (Figure 7). For this bearing and the following ones, the location of the thermocouples is at 25% and 75% of the pad arc, at 50% of the axial length, while the radial distance from the sliding surface is compliant with API 670 requirements [23]. In the following schemes, the direction of the shaft rotation is indicated as seen from the side opposite to the driver side.
The Direct Lube Rocker Pivot bearing ( Figure 5a) is a high-speed 5-pad TPJB that was designed with the aim of reaching high peripheral speeds (>100 m/s). The pads are connected to the bearing housing by means of a cylindrical pivot ( Figure 6). The pad arc geometry and the particular scheme of the lubrication layout were defined through an optimization process to target the required static and dynamic performance in the entire speed range. Each pad is instrumented with two thermocouples (Figure 7). For this bearing and the following ones, the location of the thermocouples is at 25% and 75% of the pad arc, at 50% of the axial length, while the radial distance from the sliding surface is compliant with API 670 requirements [23].   In the following schemes, the direction of the shaft rotation is indicated as seen from the side opposite to the driver side.
The Direct Lube Rocker Pivot bearing ( Figure 5a) is a high-speed 5-pad TPJB that was designed with the aim of reaching high peripheral speeds (>100 m/s). The pads are connected to the bearing housing by means of a cylindrical pivot ( Figure 6). The pad arc geometry and the particular scheme of the lubrication layout were defined through an optimization process to target the required static and dynamic performance in the entire speed range. Each pad is instrumented with two thermocouples (Figure 7). For this bearing and the following ones, the location of the thermocouples is at 25% and 75% of the pad arc, at 50% of the axial length, while the radial distance from the sliding surface is compliant with API 670 requirements [23].  The Flooded Rocker Pivot bearing (Figure 5b) is the standard product for all the applications that do not require high-speed operating range (<80 m/s). The 5 pads are equipped with a cylindrical pivot ( Figure 6) and fed with lubricant through five holes in the bearing housing. The oil fills the housing internal chamber, and the flow rate is set by varying the clearance between rotor and oil seals. This design allows to have an easier oil layout, but with less thermal exchange between oil and pad. The lower pads are instrumented with two thermocouples each while the thermal behavior of the three upper pads is assessed through a thermocouple placed at 75% of the pad arc ( Figure 8).
The Flooded Ball & Socket Pivot bearing ( Figure 5c) is one of the bearings adopted in large centrifugal compressor applications that do not require high-speed operating range (<80 m/s). The 4 pads are equipped with a ball-and-socket type pivot ( Figure 6) and fed with lubricant through spray bars attached to the bearing housing. The oil fills the housing internal chamber, and the flow rate is set by varying the spray bar holes diameter and the clearance between rotor and oil seals. Again, the lower pads are equipped with two thermocouples and the upper pads with one thermocouple (Figure 9). varying the clearance between rotor and oil seals. This design allows to have an easier oil layout, but with less thermal exchange between oil and pad. The lower pads are instrumented with two thermocouples each while the thermal behavior of the three upper pads is assessed through a thermocouple placed at 75% of the pad arc ( Figure 8). The Flooded Ball & Socket Pivot bearing ( Figure 5c) is one of the bearings adopted in large centrifugal compressor applications that do not require high-speed operating range (<80 m/s). The 4 pads are equipped with a ball-and-socket type pivot ( Figure 6) and fed with lubricant through spray bars attached to the bearing housing. The oil fills the housing internal chamber, and the flow rate is set by varying the spray bar holes diameter and the clearance between rotor and oil seals. Again, the lower pads are equipped with two thermocouples and the upper pads with one thermocouple (Figure 9).

Results
The most relevant experimental results of the three tested bearing configurations are presented in this section. The bearings test campaign was designed in order to investigate the performance of the bearings in a wide range of the possible operating conditions in terms of applied load, peripheral speed bearing configuration, oil flow, and oil inlet temperature:  The Flooded Ball & Socket Pivot bearing ( Figure 5c) is one of the bearings adopted in large centrifugal compressor applications that do not require high-speed operating range (<80 m/s). The 4 pads are equipped with a ball-and-socket type pivot ( Figure 6) and fed with lubricant through spray bars attached to the bearing housing. The oil fills the housing internal chamber, and the flow rate is set by varying the spray bar holes diameter and the clearance between rotor and oil seals. Again, the lower pads are equipped with two thermocouples and the upper pads with one thermocouple ( Figure 9).

Results
The most relevant experimental results of the three tested bearing configurations are presented in this section. The bearings test campaign was designed in order to investigate the performance of the bearings in a wide range of the possible operating conditions in terms of applied load, peripheral speed bearing configuration, oil flow, and oil inlet temperature:

Results
The most relevant experimental results of the three tested bearing configurations are presented in this section. The bearings test campaign was designed in order to investigate the performance of the bearings in a wide range of the possible operating conditions in terms of applied load, peripheral speed bearing configuration, oil flow, and oil inlet temperature: In the following sections, the results relative to a selected sub-set are presented. More specifically, the results related to two different applied static load configurations for each specific bearing are compared. The load conditions were chosen, taking into account the design load conditions of the machines (centrifugal compressor, steam turbines) equipped with each specific bearing type. The comparison was carried out considering the static (eccentricity, maximum pad metal temperature, power losses) and dynamic (asynchronous stiffness coefficients, synchronous stiffness, and damping coefficients) results. An uncertainty assessment on the dynamic system was performed and shown in previous works [22].
As for the industrial best-practice, before introducing a new bearing design in turbomachines, a component level test of the bearing must be performed to preliminarily validate the dynamic and static performance, thus reducing the associated risk in the machine design. The operating conditions presented in the paper are the design conditions of the specific turbomachines that adopt such bearing solutions.
The Direct Lube Rocker Pivot bearing was tested with a constant oil flow value of 450 L/min that represented the required oil flow to target the desired pad temperature values (lower than 90 • C) at bearing design speed (110 m/s).
The Flooded Rocker Pivot bearing was tested with an oil flow nominal value, equal to 213 L/min, representing the required value at bearing design speed (90 m/s) and with an oil inlet temperature of 40 • C.
The Flooded Ball & Socket 4-pad bearing was tested with an oil flow value of 160 L/min (required value at 90 m/s) and with an oil inlet temperature of 40 • C.

The Bump Test Results
The bump test results (Figures 10-12) illustrate the polygonal clearance profile of the bearing realized by closing the gap between the rotor and the pads along all directions with a rotating force of 5 kN, compared to the theoretical circles representing the minimum and maximum bearing assembly clearance values. The clearance curves at both proximity probes measurement planes, obtained after the iterative procedure of alignment, are almost superimposed, so, for clarity's sake, only the average curve is shown.  It is worth noting how the angular offset of pivots of the Direct Lube Rocker Pivot bearing ( Figure 10) is clearly visible through the rotated shape of the pentagon. The regularity of the pentagonal shapes and its position with respect to the theoretical minimum and maximum clearance circles testifies to the good quality of the pads manufacturing. Figure 11 shows the clearance profile for the Flooded Rocker Pivot bearing. As for the previous bearing, the angular offset of the pivot determines the rotated shape of the pentagon. The irregular shape of the pentagonal figure can be ascribed to a large misalignment between the upper and lower semi-housings entirely due to the clearance of the alignment pins.   It is worth noting how the angular offset of pivots of the Direct Lube Rocker Pivot bearing ( Figure 10) is clearly visible through the rotated shape of the pentagon. The regularity of the pentagonal shapes and its position with respect to the theoretical minimum and maximum clearance circles testifies to the good quality of the pads manufacturing. Figure 11 shows the clearance profile for the Flooded Rocker Pivot bearing. As for the previous bearing, the angular offset of the pivot determines the rotated shape of the pentagon. The irregular shape of the pentagonal figure can be ascribed to a large misalignment between the upper and lower semi-housings entirely due to the clearance of the alignment pins.
The Flooded Ball & Socket Pivot bearing measured profile is illustrated in Figure 12. The square shape produced by the four-pad bearing is regular, denoting the good quality of the pads manufacturing. It is worth noting that there is a little misalignment between the upper semi-housing (slightly moved to the left) and the lower one (slightly moved to the right). The entity of the misalignment is comprised in the design clearance of the alignment pins.
3.1.2. The Shaft Center Eccentricity Figure 13 shows the shaft center position of the Direct Lube Rocker Pivot bearing as function of the rotational speed for the two load cases (0.8, 1.7 MPa) using the nominal The Flooded Ball & Socket Pivot bearing measured profile is illustrated in Figure 12. The square shape produced by the four-pad bearing is regular, denoting the good quality of the pads manufacturing. It is worth noting that there is a little misalignment between the upper semi-housing (slightly moved to the left) and the lower one (slightly moved to the right). The entity of the misalignment is comprised in the design clearance of the alignment pins. Figure 13 shows the shaft center position of the Direct Lube Rocker Pivot bearing as function of the rotational speed for the two load cases (0.8, 1.7 MPa) using the nominal maximum clearance circle as reference. As the speed increases, the shaft moves towards the bearing center along an almost vertical line, as expected for tilting pad journal bearings. As the load increases, the shaft centerline is characterized by higher eccentricity values and it is shifted laterally in the journal rotation direction. Machines 2021, 9, x FOR PEER REVIEW 13 of 34 Figure 13. Direct Lube Rocker Pivot bearing shaft centerline with detail on the right. Figure 14 shows the shaft center location of the Flooded Rocker Pivot bearing as function of the rotational speed for the two load cases using the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an inclined line but at high speed the center moves off the regular trend and under the higher load, above 4000 rpm, it shifts horizontally. For the higher load case, as for the previous bearing, higher eccentricities of the shaft centerline are found with respect to the low load case at corresponding speed values.  Figure 15 shows the shaft center location of the Flooded Ball & Socket Pivot bearing as function of the rotational speed for the two load cases using as reference the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an almost vertical line but above 4000 rpm the center has an apparent horizontal shift to the left. The load increase has also the effect of shifting the shaft center downwards and slightly to the right.  Figure 14 shows the shaft center location of the Flooded Rocker Pivot bearing as function of the rotational speed for the two load cases using the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an inclined line but at high speed the center moves off the regular trend and under the higher load, above 4000 rpm, it shifts horizontally. For the higher load case, as for the previous bearing, higher eccentricities of the shaft centerline are found with respect to the low load case at corresponding speed values.  Figure 14 shows the shaft center location of the Flooded Rocker Pivot bearing as function of the rotational speed for the two load cases using the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an inclined line but at high speed the center moves off the regular trend and under the higher load, above 4000 rpm, it shifts horizontally. For the higher load case, as for the previous bearing, higher eccentricities of the shaft centerline are found with respect to the low load case at corresponding speed values.  Figure 15 shows the shaft center location of the Flooded Ball & Socket Pivot bearing as function of the rotational speed for the two load cases using as reference the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an almost vertical line but above 4000 rpm the center has an apparent horizontal shift to the left. The load increase has also the effect of shifting the shaft center downwards and slightly to the right.  Figure 15 shows the shaft center location of the Flooded Ball & Socket Pivot bearing as function of the rotational speed for the two load cases using as reference the nominal maximum clearance circle. The shaft moves towards the bearing center as speed increases along an almost vertical line but above 4000 rpm the center has an apparent horizontal shift to the left. The load increase has also the effect of shifting the shaft center downwards and slightly to the right.

The Shaft Center Eccentricity
At low rotational speed, the shaft center of the Flooded Ball & Socket Pivot bearing is outside the nominal maximum clearance circle but inside the bump test envelope. This can be explained with the static shaft sink value (s) evaluated according to the geometric expression [24]: with c r and Θ P representing, respectively, the bearing radial clearance and the angle between the lower pads pivot position and the vertical direction downwards. Table 5 shows the geometric shaft sink values for the three tested bearings.
with and representing, respectively, the bearing radial clearance and the angle between the lower pads pivot position and the vertical direction downwards. Table 5 shows the geometric shaft sink values for the three tested bearings. As shown in Table 5, the 4-pad Flooded Ball & Socket Pivot bearing is characterized by higher values with respect to the two 5-pad solutions due to its higher load angle . Another noteworthy aspect is the horizontal shift of the shaft centerline under static load variation observed above 4000 rpm. At that speed, the circumferential Reynolds Number = ρωRcr/μ, where ρ is the mass density, ω the angular speed, R the bearing inner radius, and μ the dynamic viscosity, is higher than the one indicating the onset of turbulence [25]. The adopted formulation is the one used to globally evaluate the bearing flow regime in industrial practice tools. Such a transition affects also other static and dynamic characteristics as reported in the following sections.

The Pad Temperatures
The pad temperatures of the Direct Lube Rocker Pivot bearing (Figure 16 and Figure  17) are characterized by a non-linear trend with speed, with a parabolic trend for the three upper pads and a more complex trend for the two lower loaded pads. The results for the 0.8 and 1.7 MPa tests are shown, respectively, in Figure 16 a), b) and Figure 17 a)   As shown in Table 5, the 4-pad Flooded Ball & Socket Pivot bearing is characterized by higher values with respect to the two 5-pad solutions due to its higher load angle Θ P .
Another noteworthy aspect is the horizontal shift of the shaft centerline under static load variation observed above 4000 rpm. At that speed, the circumferential Reynolds Number = ρωRcr/µ, where ρ is the mass density, ω the angular speed, R the bearing inner radius, and µ the dynamic viscosity, is higher than the one indicating the onset of turbulence [25]. The adopted formulation is the one used to globally evaluate the bearing flow regime in industrial practice tools. Such a transition affects also other static and dynamic characteristics as reported in the following sections.

The Pad Temperatures
The pad temperatures of the Direct Lube Rocker Pivot bearing (Figures 16 and 17) are characterized by a non-linear trend with speed, with a parabolic trend for the three upper pads and a more complex trend for the two lower loaded pads. The results for the 0.8 and 1.7 MPa tests are shown, respectively, in Figure 16a   For the high load condition, the temperature differences among the loaded and unloaded pads are higher than in the low load case due to the higher eccentricity of the former one. The difference is less marked at 0.25 offset probe locations where the hydrodynamic film is quite far from its minimum thickness point. Figure 18 and Figure 19 show the pad temperatures of the Flooded Rocker Pivot bearing as function of speed. Refer to Figure 8 for thermocouple position.  For the high load condition, the temperature differences among the loaded and unloaded pads are higher than in the low load case due to the higher eccentricity of the former one. The difference is less marked at 0.25 offset probe locations where the hydrodynamic film is quite far from its minimum thickness point. Figures 18 and 19 show the pad temperatures of the Flooded Rocker Pivot bearing as function of speed. Refer to Figure 8   For the high load condition, the temperature differences among the loaded and unloaded pads are higher than in the low load case due to the higher eccentricity of the former one. The difference is less marked at 0.25 offset probe locations where the hydrodynamic film is quite far from its minimum thickness point. Figure 18 and Figure 19 show the pad temperatures of the Flooded Rocker Pivot bearing as function of speed. Refer to Figure 8 for thermocouple position. For the three upper pads, the temperature increases non-linearly with the speed, with an almost parabolic trend and the static load has a minor impact. The two lower and most loaded pads have more complex trends, markedly different from one another and mainly non-monotonic. Higher temperature values are measured at the higher offset probe locations. Moreover, Pad A exhibits higher temperature at mid-range speeds where the laminar to turbulent transition starts to occur. As the load increases the temperatures of the lower pads increase with a maximum of about 20% for pad A, at the higher offset probe For the three upper pads, the temperature increases non-linearly with the speed, with an almost parabolic trend and the static load has a minor impact. The two lower and most loaded pads have more complex trends, markedly different from one another and mainly non-monotonic. Higher temperature values are measured at the higher offset probe locations. Moreover, Pad A exhibits higher temperature at mid-range speeds where the laminar to turbulent transition starts to occur. As the load increases the temperatures of the lower pads increase with a maximum of about 20% for pad A, at the higher offset probe location. Figures 20 and 21 show the pad temperatures of the Flooded Ball & Socket Pivot bearing as function of speed. Refer to Figure 9 for thermocouple position. For the three upper pads, the temperature increases non-linearly with the speed, with an almost parabolic trend and the static load has a minor impact. The two lower and most loaded pads have more complex trends, markedly different from one another and mainly non-monotonic. Higher temperature values are measured at the higher offset probe locations. Moreover, Pad A exhibits higher temperature at mid-range speeds where the laminar to turbulent transition starts to occur. As the load increases the temperatures of the lower pads increase with a maximum of about 20% for pad A, at the higher offset probe location. Figure 20 and Figure 21 show the pad temperatures of the Flooded Ball & Socket Pivot bearing as function of speed. Refer to Figure 9 for thermocouple position.  In this case, the pad temperatures increase non-linearly with speed. In low load conditions, the lower pads (Figure 20a) are characterized by almost coincident monotonic trends with speed while in the higher load condition (Figure 20b), the lateral movement of the shaft center towards the right determines higher pad temperature read by the TC-B2 sensor placed in the most loaded pad with respect to the other lower pad. Differences can be neglected for the lower offset probe locations ( Figure 21).
The temperatures of the upper pads are almost unaffected by the load intensity (Figure 20).

Power Losses
The mechanical power losses were derived from the measured values of torque and rotational speed. The tested bearing power losses were obtained subtracting the rolling bearings calculated power losses from the mechanical power. Figure 22 shows the trend of the power losses, respectively, at 0.8 MPa and 1.7 MPa specific bearing load values for the Direct Lube Rocker Pivot bearing. The two power losses curves are characterized by an analogous trend up to 6000 rpm (88 m/s), then for the higher load condition, the curve exhibits another huge increase up to 7800 rpm (about 110 m/s) while for the low load conditions, the slope of the power loss curve is reduced. This particular behavior was not observed in the other test campaigns performed on In this case, the pad temperatures increase non-linearly with speed. In low load conditions, the lower pads (Figure 20a) are characterized by almost coincident monotonic trends with speed while in the higher load condition (Figure 20b), the lateral movement of the shaft center towards the right determines higher pad temperature read by the TC-B2 sensor placed in the most loaded pad with respect to the other lower pad. Differences can be neglected for the lower offset probe locations ( Figure 21).
The temperatures of the upper pads are almost unaffected by the load intensity ( Figure 20).

Power Losses
The mechanical power losses were derived from the measured values of torque and rotational speed. The tested bearing power losses were obtained subtracting the rolling bearings calculated power losses from the mechanical power. Figure 22 shows the trend of the power losses, respectively, at 0.8 MPa and 1.7 MPa specific bearing load values for the Direct Lube Rocker Pivot bearing. The two power losses curves are characterized by an analogous trend up to 6000 rpm (88 m/s), then for the higher load condition, the curve exhibits another huge increase up to 7800 rpm (about 110 m/s) while for the low load conditions, the slope of the power loss curve is reduced. This particular behavior was not observed in the other test campaigns performed on flooded bearings where the speed did not exceed 6000 rpm and the main factor determining the power losses values was only the rotor speed with negligible differences between different load conditions (Figures 23 and 24). In the latter cases the power losses increase with the speed can be observed, and no deviations are visible in respect to the exponential trend as we can expect in normal operating conditions.

Dynamic Performance
In the present section, the dynamics results are shown in terms of asynchronous and synchronous coefficient.

Asynchronous Coefficients
Examples of the plots of asynchronous dynamic coefficients as function of excitation frequency are shown in Figures 25 and 26. In particular, direct stiffness and damping coefficients K xx , K yy , C xx , and C yy , for the Direct Lube Rocker Pivot bearing are reported in this section. The plots of the other coefficients can be found in Appendix A (Figures A1-A10). For each term, the measured stiffness at each excitation frequency is shown and compared with the line of best fit. Each picture presents the results of the two tested load conditions for three different speed values. In general, the tests have indicated a negligible influence of load on the power losses except for very high speeds, where turbulence effects have been observed, and a high load condition, as shown by the Flooded Rocker Pivot.

Dynamic Performance
In the present section, the dynamics results are shown in terms of asynchronous and synchronous coefficient.

Asynchronous Coefficients
Examples of the plots of asynchronous dynamic coefficients as function of excitation frequency are shown in Figures 25 and 26. In particular, direct stiffness and damping coefficients Kxx, Kyy, Cxx, and Cyy, for the Direct Lube Rocker Pivot bearing are reported in this section. The plots of the other coefficients can be found in Appendix A ( Figure A1-A10). For each term, the measured stiffness at each excitation frequency is shown and compared with the line of best fit. Each picture presents the results of the two tested load conditions for three different speed values.  It can be noticed that the asynchronous coefficients trend is well represented through a linear interpolation and it is slightly influenced by frequency.
The influence of speed and static load will be more apparent in the plots of the synchronous coefficients in the next section but here also one can see that while the direct stiffness coefficients are more influenced by load, the direct damping ones are more influenced by speed.

Synchronous Stiffness Coefficients
The synchronous stiffness coefficients were evaluated by averaging the asynchronous values at the excitation frequencies approximately equal to 0.8 and 1.2 the rotational frequency.
The dynamic results for the Direct Lube Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 27 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 28.  It can be noticed that the asynchronous coefficients trend is well represented through a linear interpolation and it is slightly influenced by frequency.
The influence of speed and static load will be more apparent in the plots of the synchronous coefficients in the next section but here also one can see that while the direct stiffness coefficients are more influenced by load, the direct damping ones are more influenced by speed.

Synchronous Stiffness Coefficients
The synchronous stiffness coefficients were evaluated by averaging the asynchronous values at the excitation frequencies approximately equal to 0.8 and 1.2 the rotational frequency.
The dynamic results for the Direct Lube Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 27 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 28. It can be noticed that the asynchronous coefficients trend is well represented through a linear interpolation and it is slightly influenced by frequency.
The influence of speed and static load will be more apparent in the plots of the synchronous coefficients in the next section but here also one can see that while the direct stiffness coefficients are more influenced by load, the direct damping ones are more influenced by speed.

Synchronous Stiffness Coefficients
The synchronous stiffness coefficients were evaluated by averaging the asynchronous values at the excitation frequencies approximately equal to 0.8 and 1.2 the rotational frequency.
The dynamic results for the Direct Lube Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 27 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 28.  The asymmetric characteristics of the 5-pad-LBP bearing determines the anisotropy behavior with higher Kyy terms with respect to Kxx in both configurations ( Figure 27). In the low load configuration, the dynamic direct stiffness coefficients are characterized by an increasing trend when the rotor speed is increasing. Such a trend is the result of the contribution of the upper pads that develop higher pressure profiles as the shaft eccentricity decreases with the speed. In the high load configuration, very high stiffness values are observed for low-speed values due to the noticeable contribution of the pivot stiffness to the total one. As the shaft position moves towards the center of the bearing, the direct stiffness values start to decrease until the 4000 rpm, where the laminar to turbulent transition occurs and an increasing trend of the dynamic stiffness properties with respect to speed can be observed.
As regards cross-coupling stiffness coefficients ( Figure 28) they are one order of magnitude smaller than the direct ones. Kyx has a monotonic trend, increasing with speed while Kxy has a non-monotonic trend. The two coefficients have the opposite sign below 6000 rpm in both load cases and below 3000 rpm in the higher load case.
The dynamic results for the Flooded Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 29 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 30.  The asymmetric characteristics of the 5-pad-LBP bearing determines the anisotropy behavior with higher K yy terms with respect to K xx in both configurations ( Figure 27). In the low load configuration, the dynamic direct stiffness coefficients are characterized by an increasing trend when the rotor speed is increasing. Such a trend is the result of the contribution of the upper pads that develop higher pressure profiles as the shaft eccentricity decreases with the speed. In the high load configuration, very high stiffness values are observed for low-speed values due to the noticeable contribution of the pivot stiffness to the total one. As the shaft position moves towards the center of the bearing, the direct stiffness values start to decrease until the 4000 rpm, where the laminar to turbulent transition occurs and an increasing trend of the dynamic stiffness properties with respect to speed can be observed.
As regards cross-coupling stiffness coefficients ( Figure 28) they are one order of magnitude smaller than the direct ones. K yx has a monotonic trend, increasing with speed while K xy has a non-monotonic trend. The two coefficients have the opposite sign below 6000 rpm in both load cases and below 3000 rpm in the higher load case.
The dynamic results for the Flooded Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 29 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 30. The asymmetric characteristics of the 5-pad-LBP bearing determines the anisotropy behavior with higher Kyy terms with respect to Kxx in both configurations ( Figure 27). In the low load configuration, the dynamic direct stiffness coefficients are characterized by an increasing trend when the rotor speed is increasing. Such a trend is the result of the contribution of the upper pads that develop higher pressure profiles as the shaft eccentricity decreases with the speed. In the high load configuration, very high stiffness values are observed for low-speed values due to the noticeable contribution of the pivot stiffness to the total one. As the shaft position moves towards the center of the bearing, the direct stiffness values start to decrease until the 4000 rpm, where the laminar to turbulent transition occurs and an increasing trend of the dynamic stiffness properties with respect to speed can be observed.
As regards cross-coupling stiffness coefficients ( Figure 28) they are one order of magnitude smaller than the direct ones. Kyx has a monotonic trend, increasing with speed while Kxy has a non-monotonic trend. The two coefficients have the opposite sign below 6000 rpm in both load cases and below 3000 rpm in the higher load case.
The dynamic results for the Flooded Rocker Pivot bearing in terms of synchronous direct stiffness coefficients are illustrated for the two load conditions in Figure 29 while the synchronous cross-coupling stiffness coefficients are plotted in Figure 30. As highlighted for the previous bearing, an asymmetric behavior between Kxx and Kyy coefficients is observed (Figure 29) due to the intrinsic characteristics of the 5-pad-LBP configuration. Differently from the previous case, in both low (1.3 MPa) and high (2.1 MPa) load configurations, the dynamic stiffnesses are characterized by a decreasing trend when the rotor speed is increasing. Due to the high eccentricity values in both cases, the upper pads do not develop a high-pressure film.
As regards cross-coupling stiffness coefficients (Figure 30), again, they are one order of magnitude smaller than the direct ones. The plot of the lower load conditions shows how the cross-coupling stiffnesses increase in magnitude with the speed until 5000 rpm and then decrease quickly. A similar behavior is observed for a higher load, but in this case, the peak in the cross-coupling coefficients is located close to 3000 rpm. Both coefficients are positive except below 2000 rpm for the higher load condition where they have the opposite sign.
The dynamic results for the Flooded Ball & Socket Pivot bearing in terms of synchronous direct stiffness Kxx and Kyy are shown for the two load conditions in Figure 31. The symmetric behavior of the 4-pad-LBP bearing solution determines the almost isotropic behavior of the direct stiffnesses in both configurations. In the low load configuration, the Kxx and Kyy dynamic stiffness are characterized by an almost constant trend when the rotor speed is increasing. In the high load configuration, small differences are observed between the two direction terms with the Kxx characterized by a higher value As highlighted for the previous bearing, an asymmetric behavior between K xx and K yy coefficients is observed (Figure 29) due to the intrinsic characteristics of the 5-pad-LBP configuration. Differently from the previous case, in both low (1.3 MPa) and high (2.1 MPa) load configurations, the dynamic stiffnesses are characterized by a decreasing trend when the rotor speed is increasing. Due to the high eccentricity values in both cases, the upper pads do not develop a high-pressure film.
As regards cross-coupling stiffness coefficients (Figure 30), again, they are one order of magnitude smaller than the direct ones. The plot of the lower load conditions shows how the cross-coupling stiffnesses increase in magnitude with the speed until 5000 rpm and then decrease quickly. A similar behavior is observed for a higher load, but in this case, the peak in the cross-coupling coefficients is located close to 3000 rpm. Both coefficients are positive except below 2000 rpm for the higher load condition where they have the opposite sign.
The dynamic results for the Flooded Ball & Socket Pivot bearing in terms of synchronous direct stiffness K xx and K yy are shown for the two load conditions in Figure 31. As highlighted for the previous bearing, an asymmetric behavior between Kxx and Kyy coefficients is observed (Figure 29) due to the intrinsic characteristics of the 5-pad-LBP configuration. Differently from the previous case, in both low (1.3 MPa) and high (2.1 MPa) load configurations, the dynamic stiffnesses are characterized by a decreasing trend when the rotor speed is increasing. Due to the high eccentricity values in both cases, the upper pads do not develop a high-pressure film.
As regards cross-coupling stiffness coefficients (Figure 30), again, they are one order of magnitude smaller than the direct ones. The plot of the lower load conditions shows how the cross-coupling stiffnesses increase in magnitude with the speed until 5000 rpm and then decrease quickly. A similar behavior is observed for a higher load, but in this case, the peak in the cross-coupling coefficients is located close to 3000 rpm. Both coefficients are positive except below 2000 rpm for the higher load condition where they have the opposite sign.
The dynamic results for the Flooded Ball & Socket Pivot bearing in terms of synchronous direct stiffness Kxx and Kyy are shown for the two load conditions in Figure 31. The symmetric behavior of the 4-pad-LBP bearing solution determines the almost isotropic behavior of the direct stiffnesses in both configurations. In the low load configuration, the Kxx and Kyy dynamic stiffness are characterized by an almost constant trend when the rotor speed is increasing. In the high load configuration, small differences are observed between the two direction terms with the Kxx characterized by a higher value The symmetric behavior of the 4-pad-LBP bearing solution determines the almost isotropic behavior of the direct stiffnesses in both configurations. In the low load configuration, the K xx and K yy dynamic stiffness are characterized by an almost constant trend when the rotor speed is increasing. In the high load configuration, small differences are observed between the two direction terms with the K xx characterized by a higher value that can be explained with the higher pivot stiffness in the vertical direction. A change in decrease rate can be observed in the range between 3000 and 4000 rpm where the laminar to turbulent regime transition is expected to occur.
As regards cross-coupling stiffness coefficients (Figure 32), again, they are one order of magnitude smaller than the direct ones and have a non-monotonic trend with speed. In almost the entire speed range, they have the opposite sign.
Machines 2021, 9, x FOR PEER REVIEW 23 of 34 that can be explained with the higher pivot stiffness in the vertical direction. A change in decrease rate can be observed in the range between 3000 and 4000 rpm where the laminar to turbulent regime transition is expected to occur. As regards cross-coupling stiffness coefficients (Figure 32), again, they are one order of magnitude smaller than the direct ones and have a non-monotonic trend with speed. In almost the entire speed range, they have the opposite sign.

Synchronous Damping Coefficients
The synchronous damping coefficients were calculated similarly to the synchronous stiffness ones. Figures 33 and 34 show, respectively, the synchronous direct and crosscoupling damping coefficients in both load conditions, for the Direct Lube Rocker Pivot bearing.

Synchronous Damping Coefficients
The synchronous damping coefficients were calculated similarly to the synchronous stiffness ones. Figures 33 and 34 show, respectively, the synchronous direct and crosscoupling damping coefficients in both load conditions, for the Direct Lube Rocker Pivot bearing.
Machines 2021, 9, x FOR PEER REVIEW 23 of 34 that can be explained with the higher pivot stiffness in the vertical direction. A change in decrease rate can be observed in the range between 3000 and 4000 rpm where the laminar to turbulent regime transition is expected to occur. As regards cross-coupling stiffness coefficients (Figure 32), again, they are one order of magnitude smaller than the direct ones and have a non-monotonic trend with speed. In almost the entire speed range, they have the opposite sign.

Synchronous Damping Coefficients
The synchronous damping coefficients were calculated similarly to the synchronous stiffness ones. Figures 33 and 34 show, respectively, the synchronous direct and crosscoupling damping coefficients in both load conditions, for the Direct Lube Rocker Pivot bearing.  The direct damping coefficients decrease with increasing speed, with a decreasing slope, and appear slightly affected by load. Direct damping is higher in the vertical direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and for almost all speeds are of opposite sign one another. Figures 35 and 36 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Rocker Pivot bearing. The direct damping coefficients decrease with increasing speed, with a decreasing slope, and appear slightly affected by load. Direct damping is higher in the vertical direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and for almost all speeds are of opposite sign one another. Figure 35 and Figure 36 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Rocker Pivot bearing.  The direct damping coefficients decrease with increasing speed, with a decreasing slope, and appear slightly affected by load. Direct damping is higher in the vertical direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and for almost all speeds are of opposite sign one another. Figure 35 and Figure 36 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Rocker Pivot bearing. The direct damping coefficients decrease with increasing speed with a decreasing slope and are slightly affected by load. In this case, direct damping is higher in the horizontal direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and are of opposite signs except below 2000 rpm for the higher load condition where they are both negative. Figure 37 and Figure 38 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Ball & Socket Pivot The direct damping coefficients decrease with increasing speed with a decreasing slope and are slightly affected by load. In this case, direct damping is higher in the horizontal direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and are of opposite signs except below 2000 rpm for the higher load condition where they are both negative. Figures 37 and 38 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Ball & Socket Pivot bearing. The direct damping coefficients decrease with increasing speed with a decreasing slope and are slightly affected by load. In this case, direct damping is higher in the horizontal direction. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and are of opposite signs except below 2000 rpm for the higher load condition where they are both negative. Figure 37 and Figure 38 show, respectively, the synchronous direct and cross-coupling damping coefficients in both load conditions, for the Flooded Ball & Socket Pivot bearing.  The direct damping terms in the two orthogonal directions x and y, as for the stiffness ones, are similar, and they are not influenced by load. They are characterized by a decreasing trend with speed up to a rotational speed value of about 5000 rpm. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and with an opposite trend to one another and an average negative value.

The Rotordynamic Behavior
To investigate the effect of the cross-coupling on its effective damping, a comparative numerical rotordynamic analysis with the measured coefficients was performed. The rotor adopted for the evaluation is a large flexible dummy rotor built and tested in the particular configuration presented in [26]. It was realized in order to be dynamically equivalent to a large specific centrifugal compressor. The dummy rotor ( Figure 39) is a six meters length shaft, carrying five dummy disks reproducing the impeller inertial properties, two external sleeves representing the dry-gas seal rotating parts, a dummy balance drum and a dummy coupling hub. The main rotordynamic parameters are summarized in [26]. A damped eigenvalue analysis was performed for each bearing type, taking into account the experimental data relative to the static load condition nearest to the effective rotor static loads: 0. 8  The direct damping terms in the two orthogonal directions x and y, as for the stiffness ones, are similar, and they are not influenced by load. They are characterized by a decreasing trend with speed up to a rotational speed value of about 5000 rpm. The cross-coupling damping coefficients are one order of magnitude lower than the direct ones and with an opposite trend to one another and an average negative value.

The Rotordynamic Behavior
To investigate the effect of the cross-coupling on its effective damping, a comparative numerical rotordynamic analysis with the measured coefficients was performed. The rotor adopted for the evaluation is a large flexible dummy rotor built and tested in the particular configuration presented in [26]. It was realized in order to be dynamically equivalent to a large specific centrifugal compressor. The dummy rotor ( Figure 39) is a six meters length shaft, carrying five dummy disks reproducing the impeller inertial properties, two external sleeves representing the dry-gas seal rotating parts, a dummy balance drum and a dummy coupling hub. The main rotordynamic parameters are summarized in [26]. A damped eigenvalue analysis was performed for each bearing type, taking into account the experimental data relative to the static load condition nearest to the effective rotor static loads: 0. 8 numerical rotordynamic analysis with the measured coefficients was performed. The rotor adopted for the evaluation is a large flexible dummy rotor built and tested in the particular configuration presented in [26]. It was realized in order to be dynamically equivalent to a large specific centrifugal compressor. The dummy rotor ( Figure 39) is a six meters length shaft, carrying five dummy disks reproducing the impeller inertial properties, two external sleeves representing the dry-gas seal rotating parts, a dummy balance drum and a dummy coupling hub. The main rotordynamic parameters are summarized in [26]. A damped eigenvalue analysis was performed for each bearing type, taking into account the experimental data relative to the static load condition nearest to the effective rotor static loads: 0. 8 Table 6. For each bearing solution, the results in terms of synchronous modes and 1st mode logarithmic decrement are presented.  Table 6. For each bearing solution, the results in terms of synchronous modes and 1st mode logarithmic decrement are presented. It is worth noticing that the first mode frequency is unaffected by the bearing solution. The Direct Lube Rocker Pivot/Flooded Ball & Socket Pivot bearings are the ones showing the higher logarithmic decrement value, coherently with the higher direct damping values with respect to the Flooded Rocker Pivot bearing solution. These results confirm the design choice of adopting higher L/D on those rotors for which it is necessary to minimize the amplification of the first critical speed.
The contribution of direct damping and cross-coupling stiffness behavior at high speeds lead to a higher stability behavior of the Flooded Ball & Socket Pivot bearing with respect to the Direct Lube Rocker Pivot one.
The same considerations hold for the 2nd mode of the rotor ( Table 7) where none of the proposed bearing solution can be adopted to guarantee the API 617 [27] rotordynamics requirements compliance. It must be highlighted that the Flooded Rocker Pivot bearing behavior on this type of rotor is totally expected since this kind of bearing has been designed, in these particular L/D configurations, for a different type of rotor.

Discussion and Conclusions
This paper deals with the results of an extensive experimental test campaign performed on different 280 mm diameter tilting pad journal bearings through the joint effort of the University of Pisa, Baker Hughes, and AM Testing. Although the three TPJBs present many different features, some comparative observations can be made on the different or similar trends of their performances, focusing on the influence of the operating parameters and configurations.
First of all, as regards the static characteristics, the Flooded Ball & Socket Pivot bearing has the greatest shaft sink due to its geometric configuration; thus, with a lower static stiffness, especially at higher loads. The oil supply system of the Direct Lube Rocker Pivot bearing guarantees lower temperatures to the pads at the same peripheral speed of the Flooded Ball & Socket Pivot, where the same load is applied during the test. This effect is related to the cool oil supplied to the pad inlet, minimizing the recirculation of hot pad outlet oil.
All the bearings show the temperature trends of the unloaded pads increasing monotonically with speed. The trend for the loaded pads depends on the bearing type, with a monotonic increasing trend for Direct Lube Rocker Pivot bearings and Flooded Ball & Socket Pivot in the case of low applied load, with a non-monotonic trend for the Flooded Rocker Pivot bearing. Flooded bearings trends highlight a temperature peak close to 4000 rpm, especially at high load, where the transition to turbulent regime occurs. This effect confirms to use flooded bearings in medium load and medium peripherical speed applications.
The L/D ratio is one of the most influential parameters on power losses, while the influence of static load is negligible. Reducing the L/D ratio, the influence of the load on the power losses estimation increases as highlighted in the Flooded Rocker Pivot.
As far as the dynamic characteristics are concerned, for all bearings, asynchronous direct stiffness coefficients appear slightly dependent on frequency.
The Direct Lube Rocker Pivot bearing exhibits direct stiffness coefficients that increase with speed at low loads while have a minimum value at high loads and medium speed; the Flooded Rocker Pivot bearing has direct stiffness coefficients decreasing with speed, the highest vertical stiffness at high load particularly affected by speed; the Flooded Ball & Socket Pivot bearing has an isotropic direct stiffness, lower than the other bearings and slightly affected by speed. This effect suggests the use of the Flooded Ball & Socket in applications, where it is not necessary to have high stiffness but a steady value in a wide range of speed.
Cross-coupling stiffness coefficients have a nonlinear trend with speed for all tested bearings. For the Flooded Rocker Pivot bearing they have the same sign in almost all tested conditions. Vice versa both Flooded Ball & Socket Pivot bearing and Direct Lube Rocker Pivot bearing have coefficients of opposite sign over most of the tested speed range.
As regards the effect of the bearing selection on rotordynamics, the results confirm the design choice of adopting higher L/D on those rotors for which it is necessary to minimize the amplification of the first and second critical speeds.
Some observed aspects, such as turbulence effects on the bearing performance, will be, in the intention of the authors, the object of future in-depth study by means of pads equipped with advanced sensors.

Acknowledgments:
The authors acknowledge the support of Eng. Francesco Maestrale in the experimental activity.

Conflicts of Interest:
The authors declare no conflict of interest.

Appendix A
This appendix presents the plots of the asynchronous direct stiffness and damping coefficients for the flooded bearings and cross-coupling stiffness and damping coefficients for all bearings as a function of excitation frequency.