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Vibration
When
a mechanical system performs oscillations
about an equilibrium position,
caused due to the action of a disturbing
force, the system is said to be
in a state of vibration.
Vibration
Although
vibration can sometimes be used to advantage – as in cleaning and mixing
machines, presence is generally undesirable for three main reasons:
structural damage – of fatigue nature due to
cyclic fluctuation of loading
cyclic fluctuation of loading
physical discomfort – experienced by personnel
associated with the system
associated with the system
noise – vibration of air molecules
generated
by a mechanical vibration
by a mechanical vibration
Vibration Characteristics
A vibration is
characterised and assessed by three parameters:
Amplitude
– it is the maximum displacement from the central /
equilibrium position
( measured as linear or angular quantity )
( measured as linear or angular quantity )
Frequency – it is the number of cycles of
oscillations completed in a
unit interval of time
Phase
– is a measure of instant at which a
vibration passes through the
central position
(only of importance when relation between two vibrations are
considered)
Vibration Modes
This is designated by the
number of nodes in a system
Node – A
point in a vibrating system where the amplitude is 0
Antinode – A
point in a vibrating system where the amplitude
is maximum.
is maximum.
A system can vibrate with 2, 3 or more
nodes as shown below.
Forms of Mechanical
Vibration
Mechanical vibrations can occur in three forms:
Classification of Vibration
Free / Natural Vibration
If
a mechanical system is displaced from its equilibrium positionand
then released, the restoring force arising from either …spring elements as in vehicle suspension material stiffness as in torsional or bending
systems or gravitational forces as in pendulum will
cause a return towards the equilibrium position.
As
there will be an overshoot and undershoot and so on, this will result in a
vibration, called Free / Natural Vibration
In a free vibrationion., the system is said to vibrate at a natural frequency.
Classification of Vibration
Forced
Vibration
When
the mechanical system vibrates under the influence of external forces and
moments, the vibratory motion is said to be forced. Forced vibrations take
place at the frequency of exiting forces or moments.
For
example:
Firing
impulse and inertia forces from the operating cycles are the exciting forces on
the elastic shaft system.
Resonance
When
the frequency of the forced vibration coincide with the frequency of the
natural vibration of the system, a resonance condition is reached.
This results in
a build up of amplitude which
may be dangerously high
to produce great fatigue
stress and finally failure of the
material.
Harmonic
It is a vibration with frequency
multiple of the first order or fundamental frequency.
For example:
If the 1st order or the fundamental frequency is 3 cycles per sec,
the second harmonic would have a frequency of 2 x 3 = 6 c/s (Hz).
Similarly, the 3rd harmonic would have a frequency of 3 x 3 = 9 c/s (Hz).
Critical Speed
If the engine is
run at a speed where this frequency coincides with the natural frequency of the
system, resonance condition will occur.
The resonance
will produce vibrations of high amplitude. The particular engine speed at which
the resonance occurs is known as Critical Speed.
For
example:
It is planned to
install a 4L60MC engine in a vessel.
Calculation
shows hull has a natural frequency of 1.5 Hz.
This corresponds to 1.5 x 60 = 90 cycles / min.
This corresponds to 1.5 x 60 = 90 cycles / min.
If
4L60MC engine runs 117 rpm @MCR, so there is a risk of resonance at 90 rpm which is within the 1st order excitation
frequency 117 x 1= 117 c/s.
Barred Speed-range
The
high stresses associated with resonant conditions start to built up as the
engine speed approaches the critical speed, and do not come back to some safe
value until the engine speed is beyond the critical speed.
The
unsafe stresses either side of the critical speed are referred to as the flank
stresses.
The
barred speed-range of an engine is the range of speed from the beginning of
unsafe flank stresses to the dying-away of these stresses at some higher speed.
Engine must not be continuously operated at
speeds within the barred range.
Damping
In a vibratory system damping may be divided into …
External damping – separate
energy absorber unit
to offer resistance to oscillation
to offer resistance to oscillation
Internal damping – provided in the material
property
internally. It is the capacity of the
material to absorb energy.
internally. It is the capacity of the
material to absorb energy.
A dynamic
force acting on an elastic system may cause a resonant vibration.
External
dampers are used to lower the peak amplitude at near resonant condition.
Excitation sources
According to the vibration characteristics of
2-stroke slow speed diesel engines, the excitation sources are divided into four categories:
2-stroke slow speed diesel engines, the excitation sources are divided into four categories:
External moments due to inertia and gas
load
Guide force
moments
Axial Vibrations
Torsional
vibration
Axial Vibration
When
the crank throw is loaded by the gas force through the connecting rod
mechanism, the arms of the crank throw deflect in the axial direction of crankshaft, exciting axial vibrations.
In
order to counteract the influence on the hull from the axial vibration, all
engines are equipped with an axial vibration damper in the forward end of the
crankshaft.
Axial Vibration Damper
The damper
usually consists of piston moving in a cylinder. The movement of the piston
causes oil to be forced through small openings so that resistance to movement
is set up. The resistance damps out the vibration.
Torsional Vibration
The
elastic shaft system of a multi-cylinder diesel engine is acted upon by a
periodically varying torque.
This causes a
harmonic displacement of masses in the plane of rotation.
This is termed
as torsional vibration.
Torsional
vibrations are thus made up of large number of harmonics of varying amplitude
and frequency.
When
crankshaft revolves at a speed such that one of these harmonics coincide with
the natural frequency of the system, resonance occurs. The shaft is said to be at critical
speed.
Torsional Vibration
Frequency of
torsional vibration of a single mass is:
Where, q is the stiffness in N-m / radian
I is the moment of inertia of attached mass in
kg / m2
The
essence of
control is to adjust these two parameters, q and I to achieve a frequency which
does not coincide with any of the forcing frequencies.
If
controlling of q & I does not give the desired result, additional masses
must be brought into the system.
Sometimes
additional mass is in the form of damper / detuner.
The commonest
detuning and damping devices used in marine practice are viscous-fluid dampers
and spring-loaded detuners.
Torsional Vibration
Damper
Silicone Damper
It comprises of
a heavy floating ring mass A and a light outer casing B rigidly connected to the end of the vibrating shaft.
Space between
the floating mass and the casing being filled with silicon fluid.
When the shaft
rotates the inner mass A is carried round with the outer casing by the viscous drag of
the fluid and will attain the shaft rpm.
When shaft
vibrates, inertia of inner mass A does not allow to follow vibration but outer casing follows the
vibration.
It causes
shearing of silicon fluid to absorb energy of vibration and gives a large
measure of damping.
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