AN OVERVIEW OF HYDRODYNAMIC BEARINGS, THEIR DEFINITION, THEORY OF OPERATION AND TROUBLESHOOTING TIPS.
BY AMR HATEM RASHED.
Hydrodynamic bearings
(also known as fluid film bearings) are often deployed as journal bearings. As
such, they come in several types, including radial tilting pad bearings, thrust
bearings for axial displacement and journal sleeve bearings.
Journal sleeve bearings
are typically used in low-speed and low-friction applications while radial
tilting pad bearings are used for high-speed applications due to the high
amplitude of vibrations.
Thrust bearings, on the
other hand, are generally employed for axial displacement in high-speed
applications as they contain tilting pads that support high-thrust loading of
rotors.
Frictionless support
The journal bearing has
several functions. It acts as frictionless support for the rotor while it is
rotating. It cools down the rotor by transferring the heat energy generated
from the process gas to the rotor and then to the oil by convection, or from
the process steam in the case of steam turbines. Another role is to dampen
high-amplitude vibrations by means of pivoted tilting pads and an oil
stream entering the bearing, which creates an oil film between the rotor and
the bearing stationary pads.
The bearing itself
consists of the journal region of the rotor and the bearing housing, containing
the internal chamber of bearing and pivoted tilting pads. There is also a
channel for oil entrance, an oil outlet and a thrust collar in the case of
thrust bearings.
The bearing undergoes a hydrodynamic
wedge effect as the rotor spins eccentrically inside the bearing housing at
its normal operating speed. The rotor exerts a force on the oil enclosed
between the rotor and the pads according to Newton’s second law and in
accordance with oil’s incompressibility property.
The oil exerts a
reaction force equal in magnitude on the rotor resulting in raising it upwards.
This action is called the hydrodynamic or wedge effect. In other words,
the heavy rotating rotor is supported by the hydrodynamic effect (viscous
force).
The main parameter
controlling hydrodynamic bearings is called “load carrying capacity” which
determines the size of the bearing. This depends on oil pressure, temperature,
flow rate, viscosity, oil film thickness and rotating speed. The
load-carrying capacity (LCC) is directly proportional to all of those
parameters except for oil temperature, which is inversely proportional.
When oil pressure
increases, it can generate vortices and eddies inside the bearing housing which
can cause high-amplitude vibrations at a frequency equal to 0.45X of the
rotating speed (oil whirling). When oil pressure decreases, it can lower
the thickness of the oil film which can lead to a drop in the vibration damping
ability so high-amplitude vibrations can occur.
Another point to note is
that when oil temperature increases, it causes a decrease in oil viscosity
which in turn leads to low oil film thickness, low vibration damping and an
increased oil flow rate (the viscous effect will decrease).
However, when the
opposite occurs (oil temperature decreases), there is greater vibration damping
ability and a higher temperature difference between the rotor and the oil. This
equates to better cooling which is a desirable condition for machine operation.
Other operational points:
· Lowering
the rate of oil flow decreases the thickness of the oil film as well as oil
pressure. However, poor cooling of the rotor also occurs.
· An
increase in oil viscosity improves vibration damping and cooling.
· Rotational
speed is directly proportional to load-carrying capacity.
· An
increase in oil film thickness can cause vortices and eddies, but if the
thickness decreases there will be low damping and a low heat transfer rate for
rotor cooling.
Oil and vibration
Oil is controlled by
means of the oil system. The oil temperature is controlled by oil coolers to
maintain the temperature within a constant accepted range. Oil pressure control
valves maintain constant pressure. An orifice maintains a constant oil flow
rate during operation.
Vibrations are associated
with rotational speed. 1X is a synchronous harmonic frequency equal to the
speed of rotation. Imbalance can be due to mechanical factors (noted by rising
vibration as rotor speed increases) or during operation because of fouling of
process gas inside the impellers.
2X is super synchronous,
superharmonic that can be generated by misalignment or mechanical looseness.
This can best be recognized by side frequencies associated with vibration
frequency peaks.
Angular misalignment is
indicated by an axial reading and a high 1X frequency compared with 2X
frequency.
Parallel misalignment, or
offset, on the other hand, is indicated by a radial (vertical) reading and a
high 2X frequency compared to the 1X frequency.
Finally, oil whip
instability may occur if the machine is operated at or above 2X the rotor’s
critical frequency; oil whirl becomes oil whip instability as the shaft speed
passes through 2X of the critical frequency.
Author
Amr Hatem Rashed is a
Senior Turbomachinery Engineer at Abu-Qir Fertilizers Company in Alexandria,
Egypt. He has a Master degree in mechanical engineering.
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