Лаборатория компьютерного моделирования "Физика колебаний". Бутиков Е.И. - 145 стр.

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ω
±
=
µ
1 +
5
12
˜m
2
±
1
8
p
˜m
4
(4/Q)
2
ω
0
.
ω
0
˜m
min
=
2
Q
, Q
min
=
4
˜m
2
, ω
res
=
µ
1 +
5
12
˜m
2
ω
0
.
n = 2
ω
+
ω
= ˜m
2
ω
0
/4
ω
+
=
µ
1 +
13
24
˜m
2
ω
0
, ω
=
µ
1 +
7
24
˜m
2
ω
0
.
ω = ω
+
γ = 0 a
0
= 0
b
1
= 0 ω = ω
b
0
= 0 a
1
= 0
ϕ a
0
b
0
a
1
b
1
t = 0
ϕ(0) = a
0
+ a
1
, ˙ϕ(0) = ω(b
0
+ 2b
1
) ω
0
(b
0
+ 2b
1
).
ω = ω
t = 0
ϕ(0) = a
0
˙ϕ(0) = 2b
1
ω
0
= (4/3) ˜ma
0
ω
0
b
1
a
0
ϕ(0) ˙ϕ(0) = (4/3) ˜(0)ω
0
ω = ω
+
t = 0
˙ϕ(0) = ω
0
b
0