BENDIX MC-12 MODULATOR CONTROLLER ASSY Guida alla Risoluzione dei Problemi Pagina 53

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depends on the proper location of the cam in respect
to the location of the brake shoes. The transmission of
the proper force is partially determined by the effective
lever length of the cam. If the effective lever length of
the cam is too long or too short, the brake shoe force
will be correspondingly too little or too much.
It is also important that the effective lever length of
the cam remains constant as the lining wears and the
shoes have to be spread further; otherwise, the brake
performance would vary as the lining wears.
Another form of lever found in drum-brake forms of
braking systems is the brake shoe. This is one of the
simpler forms because it is easily recognized as a
beam, fulcrumed at one end on the hinge pin, which
forces the brake lining against the drum when the
brake cam force is applied to the other end.
Perhaps the least easily recognized lever in a drum
brake system is the relation of the brake drum diameter
to the tire diameter. In order to understand this fully
it must be remembered that although the brakes stop
the brake drums and wheels, it is always the tires
and road surface that stop the vehicle. This is clearly
demonstrated when quick stops are attempted on
wet or icy roads. Under these conditions the brake
equipment may still be as effi cient as ever in stopping
the wheels, but its ability to stop the vehicle quickly
diminishes because there is not suffi cient friction
between the tire and road to develop the necessary
retarding force.
Returning to the principles of leverage involved in the
relation of the tire and brake drum size, the retarding
force developed by the brake shoes acting against
the drum is working on an effective lever length of the
brake drum radius. Counteracting this is the retarding
force developed between the tire and the road, working
on an effective lever length of the rolling radius of the
tire. Since it is not practical to have brake drums as
large as the tires, the principles of leverage require
development of a greater retarding force between the
brake shoes and the drums than between the tire and
the road. Also, since a rubber tire on a smooth, dry
road surface has a higher coeffi cient of friction than
brake lining against a brake drum, it is necessary to
develop additional retarding force between the brake
shoes and brake drum in order to overcome the
difference in friction.
Deceleration
In discussing brakes, the term deceleration is often
used. This term expresses the actual rate at which
vehicle speed is reduced and usually denotes the
speed being reduced each second, in terms of miles
per hour or feet per second.
As an example as shown in Figure 6 - if a vehicle
is moving at the rate of 20 miles per hour, and one
second later its speed is only 18 miles per hour, the
vehicle has reduced its speed by two miles per hour
during one second, its deceleration rate is two miles
per hour per second.
In the same way, if a vehicle is moving at a rate of 30
feet per second, and one second later its speed is only
20 feet per second, then it is decelerating at the rate
of ten feet per second per second.
Therefore, the change in the rate of speed of a vehicle
during a slowdown or stop is expressed by fi rst stating
the rate of speed being lost, such as miles per hour or
feet per second, and then by stating the time required
for this rate of speed to be lost.
Thus, in examining the expression covering a
deceleration rate of say, “ten feet per second per
second,” the fi rst part – “ten feet per second” – is the
rate of speed being lost, and the second part – “per
second” – is the time in which the loss of ten feet per
second takes place.
If a vehicle is moving at a known rate, and is
decelerating at a known rate, the stopping time will
be the initial speed divided by the deceleration rate,
provided both the rate of speed and the deceleration
rate are expressed on the same basis. As an example
– if a vehicle is moving at the rate of 30 feet per
FIGURE 6 - DECELERATION
Leverage (continued), Deceleration
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