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MAHR - Шариковые направляющие Marmotion - 2010 Английский язык
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- 44 M a r M o t i o n . H i g h - p re c i s i o n ro t a r y s t ro k e b e a r i n g s
Mahr
5. Computation of the Rotary Stroke Bearing 5.2.2 Radial load as pure
moment
Fig. 23
The end zones of contact length e
are the most heavily loaded for both
divided and undivided contact zones.
Moment M = PR · l [Nm]
PR in N, l in m
Specific radial force
P10 = g · M [N]
g in m-1
The factor g is taken from the diagram
(Fig. 25). In the case of an undivided
contact length, the distance is Ii = 0.
Deflection to be expected at the point
of application of radial force PR:
Deflection A = l P10 R10 [m]
e
R10 in m/N from table (Fig. 27 or 28)
The deflection of the shaft is not
taken into account.
5.2.3 Uneven radial load
The ball zone next to the point of
application of the radial force is most
heavily loaded.
The specific radial force P10 is a
combination of the moment M
and the radial force PR.
Specific radial force
P10 = g · M + h · PR [N]
g in m-1, h dimensionless,
M in Nm, PR in N
The factors g and h are taken
from the diagrams (Fig. 25 and 26)
depending on the distance li.
In the case of an undivided contact
length, the distance is Ii = 0.
Fig. 24
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