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Яковенко Г.Н. Краткий курс теоретической механики
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Теоретическая механика
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ω
ω
ω
ω
ω
i
{
ω
ω
ω
ω
ω
i
}
{
F
−
F
}
F
−
F
M
O
M
O
6
=
0
6
=
0
6
=
0
M
O
M
O
M
O
O
M
O
(
R
,
M
O
)
6
=
0
i
1
i
2
i
3
V
A
=
v
(
i
2
+
i
3
)
V
B
=
v
(
i
2
+
i
3
)
V
C
=
−
v
i
3
A
B
C
r
A
=
a
i
1
r
B
=
a
i
2
r
C
=
a
i
3
V
B
=
V
A
+
[
ω
ω
ω
ω
ω
,
AB
]
,
[
ω
ω
ω
ω
ω
,
AB
]
=
0
(
V
A
=
V
B
)
,
ω
ω
ω
ω
ω
=
k
AB
=
k
(
r
B
−
r
A
)
=
k
a
(
i
2
−
i
1
)
.
ω
ω
ω
ω
ω
V
C
=
V
A
+
[
ω
ω
ω
ω
ω
,
AC
]
AC
=
r
C
−
r
A
k
=
−
v
/a
2
ω
ω
ω
ω
ω
=
(
i
1
−
i
2
)
v
/a
O
V
O
=
V
A
+
[
ω
ω
ω
ω
ω
,
AO
]
=
v
i
2
AO
=
−
r
A
=
−
a
i
1
R
=
ω
ω
ω
ω
ω
=
(
i
1
−
i
2
)
v
/a
M
O
=
V
O
=
v
i
2
r
=
1
R
2
[
R
,
M
O
]
+
λ
R
=
a
(
λ
i
1
−
λ
i
2
+
i
3
/
2)
.
x
1
=
λa
x
2
=
−
λa
x
3
=
a/
2
λ
x
1
+
x
2
=
0
x
3
=
a/
2
R
M
R
=
ω
ω
ω
ω
ω
=
(
i
1
−
i
2
)
v
/a,
M
=
V
=
(
i
2
−
i
1
)
v
/
2
.
V
=
|
M
|
=
v
/
√
2
ω
=
|
R
|
=
v
√
2
/a
i
1
i
2
i
3
i
3
G
=
−
G
i
3
F
=
F
i
2
P
=
P
i
1
r
G
=
l
i
3
r
F
=
H
i
3
r
P
=
h
i
3
M
O
O
R
=
P
i
1
+
F
i
2
−
G
i
3
,
M
O
=
−
F
H
i
1
+
P
h
i
2
.
R
2
=
P
2
+
F
2
+
G
2
,
(
R
,
M
O
)
=
P
F
(
h
−
H
)
,
[
R
,
M
O
]
=
P
Gh
i
1
+
F
Gh
i
2
+
(
P
2
h
+
F
2
H
)
i
3
r
=
P
Gh
i
1
+
F
Gh
i
2
+
(
P
2
h
+
F
2
H
)
i
3
P
2
+
F
2
+
G
2
+
λ
(
P
i
1
+
F
i
2
−
G
i
3
)
.
x
3
λ
=
(
P
2
h
+
F
2
H
)
/
{
G
(
P
2
+
F
2
+
G
2
)
}
{
x
1
,
x
2
}
x
1
=
P
(
P
2
h
+
F
2
H
+
G
2
h
)
G
(
P
2
+
F
2
+
G
2
)
,
x
2
=
F
(
P
2
h
+
F
2
H
+
G
2
H
)
G
(
P
2
+
F
2
+
G
2
)
,
x
3
=
0
,
R
=
P
i
1
+
F
i
2
−
G
i
3
R
M
R
=
√
P
2
+
F
2
+
G
2
,
M
=
P
F
(
h
−
H
)
√
P
2
+
F
2
+
G
2
.
m
V
=
˙
r
=
Q
=
m
V
=
m
˙
r
Q
=
m
V
=
m
˙
r
=
.
F
t
˙
Q
=
m
˙
V
=
m
W
=
m
¨
r
=
F
(
t
,
r
,
˙
r
)
.
(15
.
1)
t
r
V
=
˙
r
m
m
W
=
m
W
=
m
W
+
m
W
+
m
W
=
F
,
m
W
=
F
+
J
+
J
.
(15
.
2)
J
=
−
m
W
,
J
=
−
m
W
=
−
2
m
[
ω
ω
ω
ω
ω
,
V
]
,
(15
.
3)
e
3
ω
ω
ω
ω
ω
(
t
)
=
ω
(
t
)
e
3
e
2
r
=
y
e
2
f
O
e
1
e
2
e
3
J
t
ïåð
J
êîð
F
N
G
J
n
ïåð
m
J
=
−
m
W
=
−
m
W
n
−
m
W
τ
=
J
n
+
J
τ
=
mω
2
(
t
)
y
e
2
+
m
˙
ω
(
t
)
y
e
1
,
J
=
−
m
W
=
−
2
m
[
ω
ω
ω
ω
ω
,
V
]
=
2
mω
(
t
)
˙
y
e
1
F
=
−
F
e
2
sign
˙
y
G
=
−
mg
e
3
N
e
2
m
¨
y
=
mω
2
(
t
)
y
−
F
F
F
=
f
N
f
N
N
{
e
1
e
3
}
0
=
N
+
G
+
J
τ
+
J
=
N
−
mg
e
3
+
m
˙
ω
(
t
)
y
e
1
+
2
mω
(
t
)
˙
y
e
1
.
N
N
=
r
m
2
g
2
+
³
m
˙
ω
(
t
)
y
+
2
mω
(
t
)
˙
y
´
2
N
m
¨
y
=
ω
2
(
t
)
y
−
f
r
g
2
+
³
˙
ω
(
t
)
y
+
2
ω
(
t
)
˙
y
´
2
sign
˙
y
{
F
,
−
F
}
F
r
N
m
1
m
2
m
N
r
1
r
C
C
r
2
...
F
âíåøí
-
F
âíóòð
F
âíóòð
r
C
=
1
m
N
X
i
=1
m
i
r
i
,
m
=
N
X
i
=1
m
i
.
(16
.
1)
r
=
N
P
i
=1
λ
i
r
i
λ
i
≥
0
N
P
i
=1
λ
i
=
1
λ
i
=
m
i
/m
Q
=
N
X
i
=1
m
i
V
i
=
N
X
i
=1
m
i
˙
r
i
.
(16
.
2)
m
r
C
=
N
P
i
=1
m
i
r
i
t
m
˙
r
C
=
m
V
C
=
N
X
i
=1
m
i
˙
r
i
=
N
X
i
=1
m
i
V
i
=
Q
,
(16
.
3)
Q
=
m
V
C
.
(16
.
4)
t
m
¨
r
C
=
m
˙
V
C
=
N
X
i
=1
m
i
¨
r
i
=
N
X
i
=1
m
i
˙
V
i
=
˙
Q
,
m
i
˙
V
i
=
m
¨
r
i
=
F
i
+
F
i
˙
Q
=
m
˙
V
C
=
m
W
C
=
m
¨
r
C
=
N
X
i
=1
m
i
¨
r
i
=
N
X
i
=1
m
i
˙
V
i
=
N
X
i
=1
(
F
i
+
F
i
)
N
P
i
=1
F
i
=
0
˙
Q
=
R
,
m
W
C
=
R
,
(16
.
5)
R
R
=
N
P
i
=1
F
i
R
z
R
z
Q
z
=
V
z
=
R
R
R
R
=
−
2
N
X
i
=1
m
i
[
ω
ω
ω
ω
ω
,
V
i
]
=
−
2[
ω
ω
ω
ω
ω
,
N
X
i
=1
m
i
V
i
]
=
−
2
m
[
ω
ω
ω
ω
ω
,
V
C
]
.
R
R
=
−
m
W
C
R
=
−
2
m
[
ω
ω
ω
ω
ω
,
V
C
]
R
=
−
m
W
C
O
K
O
=
N
X
i
=1
[
r
i
,
m
i
V
i
]
,
(17
.
1)
r
i
O
i
K
O
O
A
O
K
O
OA
r
i
m
i
V
i
O
A
K
A
=
K
O
−
[
O
A,
Q
]
,
(17
.
2)
t
˙
K
O
=
N
X
i
=1
[
r
i
,
m
i
˙
V
i
]
+
N
X
i
=1
[
˙
r
i
,
m
i
V
i
]
,
m
i
˙
V
i
=
F
i
+
F
i
˙
r
i
=
V
i
−
V
O
˙
K
O
=
N
X
i
=1
[
r
i
,
F
i
+
F
i
]
+
N
X
i
=1
[
V
i
−
V
O
,
m
i
V
i
]
,
‹
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2
3
4
5
6
7
8
...
12
13
›