Лаборатория компьютерного моделирования "Физика колебаний". Бутиков Е.И. - 86 стр.

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∗∗
ω = 0.25 ω
0
ω = 4 ω
0
ω = 4 ω
0
∗∗
ω = 0.125 ω
0
ω = 0.5 ω
0
ω = 1.5 ω
0
ω = 2 ω
0
ω = 6 ω
0
¨ϕ + 2γ ˙ϕ + ω
2
0
ϕ = ω
2
0
φ
0
sin ωt.
ϕ(t) = a sin(ωt + δ).
a δ
a(ω) =
ω
2
0
φ
0
p
(ω
2
0
ω
2
)
2
+ 4γ
2
ω
2
, tan δ =
2γω
ω
2
0
ω
2
.
ω
res
ω
res
=
q
ω
2
0
2γ
2
ω
0
µ
1
γ
2
ω
2
0
= ω
0
µ
1
1
4Q
2
.
γ <
2 ω
0
γ ¿ ω
0
a
max
=
ω
2
0
φ
0
2γ
p
ω
2
0
γ
2
ω
0
φ
0
2γ
=
0
.
Q Q = ω
0
/(2γ)
= ωa(ω) =
ω
2
0
φ
0
p
(ω
2
0
ω)
2
+ 4γ
2
.
max
ω = ω
0
max
= ωa(ω
0
) =
ω
2
0
φ
0
2γ
= ω
0
0
.