26
2006. 2
. . , . .
-
, -
[1]:
cos . cos
sin sin
1 1
c r
c r
y x
. sin sin
cos cos
2 1
2 1
c z
r w
c z
r w
y
x (1)
: 1 cos
2 2
2 2 1 2
2 w r z c z
w
w x y .(2)
w
wmin 12zec z min
wmax 12ze c z max.
. 1 r w
2
). 1
:
2 2 2 1 2 1 2
0 2 1
2 d r z c
w . . (5)
w
wn wt, -
.
n n w n w n
n
wn w x x y y ,
n – , -
; |n| – .
,
1 cos 2 1
1 cos 1
2 2 2
1 c c z
z c z c r z
wn . (6)
wn z
r
wn 12 wn 12r z .
y y x x t
w w w
w ,
– , ; | | – -
.
, -
, | | = |n|,
1 cos 2 1
1 sin 1
2 2
1 c c z
z c r z
wt . (7)
. 1.
r w
2 1
1,0 2
9 4
9 6
9 8
9 2,0
3,0 w
1r
2 = 2,0
= 2,5 = 3,0
2
0
2 / d w w
2
0
2 2 2
1 2 cos 1
2 /
d z zc c z
r . (3)
z c z c r
w 2 2 2 3
1 . (4)
2 9
4 9
6 9
8 9 w
r
t 1
2
-1,0 0 1,0
-2,0 = 2,0 = 2,5 = 3,0
2 9
4 9
6 9
8 9 w
r
n 1
2
1,0 3,0 5,0
-1,0 0
= 2,0 = 2,5 = 3,0
. 2.
r wn
2
1 r
wt
2 1
27 -
, :
1
1 12
2
1r z wt r z .
r wn
2
1 r
wt
2 1
. 2.
- (1)–(7)
-
( ) -
[2].
1. ., ., . -
,
. // . , 2003. 3-4.
. 93-99.
2. .
// . . .- . ,
2004. 4. . 23-26.
- i
. -
i.
Summary
Theoretical dependences for definition of tops of a rotor of building road machines with the planetary movement are received. Allowing to calculate centrifugal forces of inertia.
621.926.2
3.06.05 .
. .
- , - .
(
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