1.2 Engine, transmission and body structure mountings 1.2.1 Inherent engine vibrations The vibrations originating within the engine are caused by both the cyclic acceleration of the reci
Trang 1floor, a rule or tape is used to measure the distances
between centres both transversely and diagonally
These values are then chalked along their respective
lines Misalignment or error is observed when a
pair of transverse or diagonal dimensions differ
and further investigation will thus be necessary
Note that transverse and longitudinal
dimen-sions are normally available from the
manufac-turer's manual and differences between paired
diagonals indicates lozenging of the framework
due to some form of abnormal impact which has
previously occurred
1.2 Engine, transmission and body structure
mountings
1.2.1 Inherent engine vibrations
The vibrations originating within the engine are
caused by both the cyclic acceleration of the
reci-procating components and the rapidly changing
cylinder gas pressure which occurs throughout
each cycle of operation
Both the variations of inertia and gas pressure forces generate three kinds of vibrations which are transferred to the cylinder block:
1 Vertical and/or horizontal shake and rock
2 Fluctuating torque reaction
3 Torsional oscillation of the crankshaft 1.2.2 Reasons for flexible mountings
It is the objective of flexible mounting design to cope with the many requirements, some having conflicting constraints on each other A list of the duties of these mounts is as follows:
1 To prevent the fatigue failure of the engine and gearbox support points which would occur if they were rigidly attached to the chassis or body structure
2 To reduce the amplitude of any engine vibration which is being transmitted to the body structure
3 To reduce noise amplification which would occur
if engine vibration were allowed to be transferred directly to the body structure
Fig 1.9 Body underframe alignment checks
Trang 24 To reduce human discomfort and fatigue by
partially isolating the engine vibrations from
the body by means of an elastic media
5 To accommodate engine block misalignment
and to reduce residual stresses imposed on the
engine block and mounting brackets due to
chassis or body frame distortion
6 To prevent road wheel shocks when driving
over rough ground imparting excessive rebound
movement to the engine
7 To prevent large engine to body relative
move-ment due to torque reaction forces, particularly
in low gear, which would cause excessive
mis-alignment and strain on such components as
the exhaust pipe and silencer system
8 To restrict engine movement in the fore and aft
direction of the vehicle due to the inertia of the
engine acting in opposition to the accelerating
and braking forces
1.2.3 Rubber flexible mountings (Figs 1.10, 1.11
and 1.12)
A rectangular block bonded between two metal
plates may be loaded in compression by squeezing
the plates together or by applying parallel but
opposing forces to each metal plate On
compres-sion, the rubber tends to bulge out centrally from
the sides and in shear to form a parallelogram
(Fig 1.10(a))
To increase the compressive stiffness of the
rubber without greatly altering the shear stiffness,
an interleaf spacer plate may be bonded in between
the top and bottom plate (Fig 1.10(b)) This
inter-leaf plate prevents the internal outward collapse of
the rubber, shown by the large bulge around the
sides of the block, when no support is provided,
whereas with the interleaf a pair of much smaller
bulges are observed
When two rubber blocks are inclined to each other
to form a `V' mounting, see Fig 1.11, the rubber will
be loaded in both compression and shear shown by the triangle of forces The magnitude of compressive force will be given by Wcand the much smaller shear force by WS This produces a resultant reaction force
WR The larger the wedge angle , the greater the proportion of compressive load relative to the shear load the rubber block absorbs
The distorted rubber provides support under light vertical static loads approximately equal in both compression and shear modes, but with heavier loads the proportion of compressive stiffness Fig 1.10 (a and b) Modes of loading rubber blocks
Fig 1.11 `V' rubber block mounting
Trang 3to that of shear stiffness increases at a much faster
rate (Fig 1.12) It should also be observed that the
combined compressive and shear loading of the
rubber increases in direct proportion to the static
deflection and hence produces a straight line graph
1.2.4 Axis of oscillation (Fig 1.13)
The engine and gearbox must be suspended so that
it permits the greatest degree of freedom when
oscillating around an imaginary centre of rotation
known as the principal axis This principal axis
produces the least resistance to engine and gearbox
sway due to their masses being uniformly
distrib-uted about this axis The engine can be considered
to oscillate around an axis which passes through
the centre of gravity of both the engine and gearbox
(Figs 1.13(a, b and c)) This normally produces an
axis of oscillation inclined at about 10±20 to the
crankshaft axis To obtain the greatest degree of
freedom, the mounts must be arranged so that they
offer the least resistance to shear within the rubber
mounting
1.2.5 Six modes of freedom of a suspended body
(Fig 1.14)
If the movement of a flexible mounted engine is
completely unrestricted it may have six modes of
vibration Any motion may be resolved into three
linear movements parallel to the axes which pass
through the centre of gravity of the engine but at
right angles to each other and three rotations about
these axes (Fig 1.14)
These modes of movement may be summarized
as follows:
Linear motions Rotational motions
longitudinal 5 Pitch
2 Horizontal lateral 6 Yaw
3 Vertical
1.2.6 Positioning of engine and gearbox mountings (Fig 1.15)
If the mountings are placed underneath the com-bined engine and gearbox unit, the centre of gravity
is well above the supports so that a lateral (side) force acting through its centre of gravity, such as experienced when driving round a corner, will cause the mass to roll (Fig 1.15(a)) This condition is undesirable and can be avoided by placing the mounts on brackets so that they are in the same plane as the centre of gravity (Fig 1.15(b)) Thus the mounts provide flexible opposition to any side force which might exist without creating a roll couple This is known as a decoupled condition
An alternative method of making the natural modes of oscillation independent or uncoupled is achieved by arranging the supports in an inclined
`V' position (Fig 1.15(c)) Ideally the aim is to make the compressive axes of the mountings meet
at the centre of gravity, but due to the weight of the power unit distorting the rubber springing the inter-section lines would meet slightly below this point Therefore, the mountings are tilted so that the compressive axes converge at some focal point above the centre of gravity so that the actual lines
of action of the mountings, that is, the direction
of the resultant forces they exert, converge on the centre of gravity (Fig 1.15(d))
The compressive stiffness of the inclined mounts can be increased by inserting interleafs between the rubber blocks and, as can be seen in Fig 1.15(e), the line of action of the mounts con-verges at a lower point than mounts which do not have interleaf support
Engine and gearbox mounting supports are normally of the three or four point configuration Petrol engines generally adopt the three point support layout which has two forward mounts (Fig 1.13(a and c)), one inclined on either side of the engine so that their line of action converges on the principal axis, while the rear mount is supported centrally at the rear of the gearbox in approximately the same plane as the principal axis Large diesel engines tend to prefer the four point support Fig 1.12 Load±deflection curves for rubber block
Trang 4arrangement where there are two mounts either side
of the engine (Fig 1.13(b)) The two front mounts
are inclined so that their lines of action pass through
the principal axis, but the rear mounts which are
located either side of the clutch bell housing are not
inclined since they are already at principal axis level
1.2.7 Engine and transmission vibrations
Natural frequency of vibration (Fig 1.16) A sprung
body when deflected and released will bounce up and
down at a uniform rate The amplitude of this cyclic movement will progressively decrease and the num-ber of oscillations per minute of the rubnum-ber mounting
is known as its natural frequency of vibration There is a relationship between the static deflec-tion imposed on the rubber mount springing by the suspended mass and the rubber's natural frequency
of vibration, which may be given by
n0p30 x Fig 1.13 Axis of oscillation and the positioning of the power unit flexible mounts
Trang 5where n0 = natural frequency of vibration
(vib/min)
x = static deflection of the rubber (m)
This relationship between static deflection and
natural frequency may be seen in Fig 1.16
Resonance Resonance is the unwanted
synchron-ization of the disturbing force frequency imposed by
the engine out of balance forces and the fluctuating cylinder gas pressure and the natural frequency of oscillation of the elastic rubber support mounting, i.e resonance occurs when
n
n0 1 where n = disturbing frequency
n0 = natural frequency Transmissibility (Fig 1.17) When the designer selects the type of flexible mounting the Theory of Transmissibility can be used to estimate critical resonance conditions so that they can be either prevented or at least avoided
Transmissibility (T) may be defined as the ratio
of the transmitted force or amplitude which passes through the rubber mount to the chassis to that of the externally imposed force or amplitude generated
by the engine:
T Ft
Fd 1
n0
2
where Ft transmitted force or amplitude
Fd imposed disturbing force or
amplitude This relationship between transmissibility and the ratio of disturbing frequency and natural frequency may be seen in Fig 1.17
Fig 1.14 Six modes of freedom for a suspended block
Fig 1.16 Relationship of static deflection and natural
frequency
Trang 6Fig 1.15 (a±e) Coupled and uncoupled mounting points
Trang 7The transmissibility to frequency ratio graph
(Fig 1.17) can be considered in three parts as follows:
Range(I) Thisistheresonancerangeandshouldbe
avoided It occurs when the disturbing frequency
is very near to the natural frequency If steel mounts
are used, a critical vibration at resonance would go
to infinity, but natural rubber limits the
trans-missibility to around 10 If Butyl synthetic rubber is
adopted, its damping properties reduce the peak
transmissibility to about 21 ¤ 2 Unfortunately, high
damping rubber compounds such as Butyl rubber
are temperature sensitive to both damping and
dynamic stiffness so that during cold weather a
noticeably harsher suspension of the engine results
Damping of the engine suspension mounting is
necessary to reduce the excessive movement of a
flexible mounting when passing through resonance,
but at speeds above resonance more vibration is
transmitted to the chassis or body structure than
would occur if no damping was provided
Range (II) This is the recommended working
range where the ratio of the disturbing frequency
to that of the natural frequency of vibration of the
rubber mountings is greater than 11 ¤ 2and the trans-missibility is less than one Under these conditions off-peak partial resonance vibrations passing to the body structure will be minimized
Range (III) This is known as the shock reduction range and only occurs when the disturbing frequency is lower than the natural frequency Generally it is only experienced with very soft rubber mounts and when the engine is initially cranked for starting purposes and so quickly passes through this frequency ratio region
Example An engine oscillates vertically on its flexible rubber mountings with a frequency of 800 vibrations per minute (vpm) With the information provided answer the following questions:
a) From the static deflection±frequency graph, Fig 1.16, or by formula, determine the natural fre-quency of vibration when the static deflection of the engine is 2 mm and then find the disturbing to naturalfrequencyratio.Commentontheseresults b) If the disturbing to natural frequency ratio is increased to 2.5 determine the natural frequency
Fig 1.17 Relationship of transmissibility and the ratio of disturbing and natural frequencies for natural rubber, Butyl rubber and steel
Trang 8of vibration and the new static deflection of the
engine Comment of these conditions
a) n0p30xp0:00230
0:0447230 670:84 vib/min
n0 800
670:84 1:193
The ratio 1.193 is very near to the resonance
condition and should be avoided by using softer
mounts
b) nn
0800n
0 2:5
; n0800
2:5 320 vib/min
Now n0p30
x thuspx 30n
0
; x 30n
0
2
32030
2
0:008789 m or 8:789 mm
A low natural frequency of 320 vib/min is well
within the insulation range, therefore from either
the deflection±frequency graph or by formula
the corresponding rubber deflection necessary is
8.789 mm when the engine's static weight bears
down on the mounts
1.2.8 Engine to body/chassis mountings
Engine mountings are normally arranged to
provide a degree of flexibility in the horizontal
longitudinal, horizontal lateral and vertical axis of
rotation At the same time they must have
suffi-cient stiffness to provide stability under shock
loads which may come from the vehicle travelling
over rough roads Rubber sprung mountings
suitably positioned fulfil the following functions:
1 Rotational flexibility around the horizontal
longitudinal axis which is necessary to allow the
impulsive inertia and gas pressure components
of the engine torque to be absorbed by rolling of
the engine about the centre of gravity
2 Rotational flexibility around both the horizontal
lateral and the vertical axis to accommodate any
horizontal and vertical shake and rock caused by
unbalanced reciprocating forces and couples
1.2.9 Subframe to body mountings (Figs 1.6 and 1.19)
One of many problems with integral body design is the prevention of vibrations induced by the engine, transmission and road wheels from being transmitted through the structure Some manufacturers adopt a subframe (Fig 1.6(a, b and c)) attached by resilient mountings (Fig 1.19(a and b)) to the body to which the suspension assemblies, and in some instances the engine and transmission, are attached The mass
of the subframes alone helps to damp vibrations
It also simplifies production on the assembly line, and facilitates subsequent overhaul or repairs
In general, the mountings are positioned so that they allow strictly limited movement of the subframe in some directions but provide greater freedom in others For instance, too much lateral freedom of a subframe for a front suspension assembly would introduce a degree of instability into the steering, whereas some freedom in vertical and longitudinal directions would improve the quality of a ride
1.2.10 Types of rubber flexible mountings
A survey of typical rubber mountings used for power units, transmissions, cabs and subframes are described and illustrated as follows:
Double shear paired sandwich mounting (Fig 1.18(a)) Rubber blocks are bonded between the jaws of a `U' shaped steel plate and a flat interleaf plate so that a double shear elastic reaction takes place when the mount is subjected to vertical load-ing This type of shear mounting provides a large degree of flexibility in the upright direction and thus rotational freedom for the engine unit about its principal axis It has been adopted for both engine and transmission suspension mounting points for medium-sized diesel engines
Double inclined wedge mounting (Fig 1.18(b)) The inclined wedge angle pushes the bonded rubber blocks downwards and outwards against the bent-up sides of the lower steel plate when loaded
in the vertical plane The rubber blocks are subjected
to both shear and compressive loads and the propor-tion of compressive to shear load becomes greater with vertical deflection This form of mounting is suitable for single point gearbox supports
Inclined interleaf rectangular sandwich mounting (Fig 1.18(c)) These rectangular blocks are
Trang 9Fig 1.18 (a±h) Types of rubber flexible mountings
Trang 10Fig 1.18 contd