análisis dinámico de estructuras en el dominio de la frecuencia
DESCRIPTION
Calculo dinámico de estructurasTRANSCRIPT
kc
�
�
A
0
0±A
T
fT = 1
fu
A2A
60km/h
Tf
h
f = 12π
√km
Δt
δΠH = 0
δ (t1, t2)
ΠH =ˆ t2
t1
(Ep − Ec)dt +ˆ t2
t1
Eddt
Ep Ec Ed
mu + cu + ku = p(t)
m
c
k
u
u
u
mu
cu
ku
p(t)
F (t)I + F (t)D + F (t)K = p(t)
m c k
{M}u + {C}u + {K}u = p(t)
u u u
t
p(x, t)
m∂2u
∂t2+
∂2
∂x2(EI
∂2u
∂x2) = p(x, t)
u
∂2
∂x2(EI
∂2v
∂x2+ c I
∂3v
∂t∂x2) + m
∂2v
∂t2+ c
∂v
∂t= p(x, t)
u(y, t)ψi(y) βi(t)
u(y, t) =∞∑i=1
ψi(y)βi(t)
ψi(y)
βi(t)
F (t)I + F (t)D + F (t)K = {p(t)}
{u}{a}i Yi(t)
{u} = [a] {Y }i
[a]{u}
M {u} + C {u} + K {u} = {p(t)}
Yi + 2DiωiYi + ω2i Yi =
Pi(t)Mi
Pi(t) = {a}Ti {p(t)}
Mi {a}Ti M {a}i
ωi
Di
{u} = {a}1 Y1 + {a}2 Y2 + ... + {a}n Yn
Δt
Δt Δt
Δt
T
Δt
ΔtT ≤ 1
10Δt
x(t)p(t)
H(Ω)P (Ω) H(Ω)P (Ω)
X(Ω)x1(t) p1(t)
x2(t) p2(t)
X1(Ω)P1(Ω)
=X2(Ω)P2(Ω)
= .........Xn(Ω)n(Ω)
= H(Ω)
X1(Ω) P1(Ω)
H(Ω)p(t)
g(t) Tp
g(t) = g(t + nTp)
Tp
g(t) = a0 +∞∑
n=1
ancos(2πnf1t) +∞∑
n=1
bnsin2π(nf1t)
f1 = 1Tp
an = 2Tp
´ Tp2
−Tp2
g(t)cos(nΩ1t)dt
bn = 2Tp
´ Tp2
−Tp2
g(t)sin(nΩ1t)dt
a0 = 1Tp
´ Tp2
−Tp2
g(t)dt
Ω1 = 2πf1
g(t) = a0 +∞∑
n=1
ancos(nΩ1t) +∞∑
n=1
bnsin(nΩ1t)
g(t)
g(t) (−Tp
2 ,Tp
2 )
g(t)g(α+0) g(α−0) α
t = 0
p0
u(t) =p0
k
(p0sinΩ1t)
u(t) =p0
k
11 − β2
sin(Ω1t)
(p0cosΩ1t)
u(t) =p0
k
11 − β2
cos(Ω1t)
β = Ω1ω
ω :Ω1 :
(p0sinΩ1t)
u(t) =p0
k
1(1 − β2)2 + (2ξβ)2
{(1 − β2)sin(Ω1t) − 2ξβcos(Ω1t)
}(p0cosΩ1t)
u(t) =p0
k
1(1 − β2)2 + (2ξβ)2
{2ξβsin(Ω1t) + (1 − β2)cos(Ω1t)
}
g(t) = a0 +∞∑
n=1
ancos(nΩ1t) +∞∑
n=1
bnsin(nΩ1t)
u(t) =a0
k+
∞∑n=1
an
k
11 − β2
n
cos(nΩ1t) +∞∑
n=1
bn
k
11 − β2
n
sin(nΩ1t)
βn = nΩ1ω
u(t) =a0
k+
∞∑n=1
an
k
1(1 − β2
n)2 + (2ξβn)2{2ξβnsin(nΩ1t) + (1 − β2
n)cos(nΩ1t)}
+∞∑
n=1
bn
k
1(1 − β2
n)2 + (2ξβn)2{(1 − β2
n)sin(nΩ1t) − 2ξβncos(nΩ1t}
=a0
k+
∞∑n=1
1k
1(1 − β2
n)2 + (2ξβn)2[{an2ξβn + bn(1 − β2
n)}
sin(nΩ1t)+
{an(1 − βn)2 − bn2ξβn
}cos(nΩ1t)]
ξξ = c
cc
sin(nΩ1t) =einΩ1t − e−inΩ1t
2i
cos(nΩ1t) =einΩ1t + e−inΩ1t
2
g(t) =∞∑
n=−∞cneinΩ1t
p = eiΩ1t
mu + cu + ku = eiΩ1t
u = e−ξωt(Acos(ωddt) + Bsin(ωdt))
ωd = ω√
1 − ξ2 ω
u = HeiΩ1t
u u u
(−mΩ21 + icΩ1 + k)HeiΩ1t = eiΩ1t
u = e−ξωt(Acos(ωdt) + Bsin(ωdt)) +1
−mΩ21 + icΩ1 + k
eiΩ1t
eiΩ1t
H(Ω1)eiΩ1t
H(Ω1) =1
−mΩ21 + icΩ1 + k
=1
k(−β2 + 2iξβ + 1)
β = Ω1ωH(Ω1)
g(t) =∞∑
n=−∞cneinΩ1t
u(t) =∞∑−∞
cnH(nΩ1)einΩ1t
cn =1Tp
ˆ Tp2
−Tp2
g(t)e−inΩ1tdt
g(t) =∞∑−∞
cneinΩ1t
cn =1Tp
ˆ Tp2
−Tp2
g(t)e−inΩ1tdt
Tp
Ω1 = 2πTp
= ΔΩ nΩ1 = Ωn = nΔΩ
cn
g(t) =∞∑−∞
cneinΩ1t =1Tp
∞∑−∞
(cnTp)eiΩnt =12π
∞∑−∞
(cnTp)eiΩntΔΩ
cnTp =ˆ Tp
2
−Tp2
g(t)e−inΩ1tdt =ˆ Tp
2
−Tp2
g(t)e−iΩntdt
Tp ΔΩ nΩ1 = Ωn = nΔΩ Ω.
cnTp = G(Ω) =ˆ ∞
−∞g(t)e−iΩtdt
g(t) =12π
ˆ ∞
−∞G(Ω)eiΩtdΩ
G(Ω) g(t)G(Ω)
∞∑−∞
cneiΩnt
u(t) =1Tp
∞∑−∞
(cnTp)H(Ωn)eiΩnt =12π
∞∑−∞
(cnTp)H(Ωn)eiΩnt�Ω
Tp
u(t) =12π
ˆ ∞
−∞G(Ω)H(Ω)eiΩtdΩ
δ(t)
δ(t) = 0 t �= 0
δ(t) t = 0
´∞−∞ δ(t)dt = 1
h(t) =12π
ˆ ∞
−∞G(Ω)H(Ω)eiΩtdΩ
´∞−∞ f(z)δ(z − t0)dt = f(t0)
G(Ω) =ˆ ∞
−∞δ(t)e−iΩtdt = 1
G(Ω) h(t)
h(t) ⇔ H(Ω)
U(Ω) u(t)
u(t) =12π
ˆ ∞
−∞U(Ω)eiΩtdΩ
U(Ω) = G(Ω)H(Ω)
g(t) h(t) g(t) ∗ h(t)
u(t) = g(t) ∗ h(t) =ˆ ∞
−∞g(τ)h(t − τ)dτ
h(τ)
g(τ)
g(τ)
U(Ω) =ˆ ∞
−∞[ˆ ∞
−∞g(τ)h(t − τ)dτ ]e−iΩtdt =
ˆ ∞
−∞[ˆ ∞
−∞h(t − τ)e−iΩtdt]g(τ)dτ
t − τ = y
U(Ω) =ˆ ∞
−∞[ˆ ∞
−∞h(y)e−iΩtdy]e−iΩτg(τ)dτ =
ˆ ∞
−∞H(Ω)e−iΩτg(τ)dτ = H(Ω)G(Ω)
U(Ω) u(t)
u(t) =12π
ˆ ∞
−∞G(Ω)H(Ω)eiΩtdΩ
Tp
G(Ω) =ˆ ∞
−∞g(t)e−iΩtdt
Ω1 = ΔΩ =2π
Tp
Tp Δt,tm = mΔt.
g(t) =ΔΩ2π
∞∑−∞
G(Ω)eiΩnt
Ωn = nΩ1
eiΩnt = einΔΩmΔt = ein 2π
TpmΔt = ein 2π
NΔtmΔt = e2πin m
N
g(tm) =ΔΩ2π
N−1∑n=0
G(Ω)e2πin mN
(N − 1)ΔΩg(t), G(Ω)
G(Ω) = Tpcn =ˆ Tp
2
−Tp2
g(t)e−iΩntdt
G(nΔΩ) = Δt
N−1∑m=0
g(mΔt)e−2πin mN
ΔΩ
Tp = NΔt
u(nΔt) =N−1∑n=0
g(nΔt)h {(m − n)Δt}Δt
g(t) h(t) Δt
g(mΔt)h(mΔt)
G(nΔΩ) =N−1∑m=0
g(mΔt)e−2πim nN
h(t)h(t)
”T0”
G(nΔΩ) H(nΔΩ)
U(nΔΩ) = G(nΔΩ)H(nΔΩ)
u(mΔt) =12π
N−1∑m=0
U(nΔΩ)e2πim nN ΔΩ
h(t)H(Ω)
H(Ω)
Tp = 1,6
Tp
mΔt m Δt = 0,1
G(nΔΩ) =N−1∑m=0
g(mΔt)e−imΔtnΔΩΔt =N−1∑m=0
g(mΔt)e−2πim nN Δt
nΔΩnΔf Δf
Δf =ΔΩ2π
=1Tp
Tp = 2πΔΩ = 1
Δf = 1, 6
ΔΩ = 1,25π Δf = 0,625
n = N2
n = N2 .
kΔΩ
G(kΔΩ) =N−1∑m=0
g(mΔt)e−2πim kN Δt
kΔΩ N ΔΩ2 lΔΩ l = N
2 + (N2 − k) = N − k
G {(N − k)ΔΩ} =N−1∑m=0
g(mΔt)e−2πim(N−k)
N Δt =
=N−1∑m=0
g(mΔt)e2πim kN Δt
n = −k
G {(−k)ΔΩ} =N−1∑m=0
g(mΔt)e2πim kN Δt
N ΔΩ2
N ΔΩ2
N ΔΩ2 = π
Δt Δt
G(Ω) =ˆ t1
0e−iΩtdt
G(Ω) =ˆ t1
0cos(Ωt)dt − i
ˆ t1
0sin(Ωt)dt =
sin(Ωt1)Ω
+ icos(Ωt1) − 1
Ω
NΔΩN ΔΩ
2
N ΔΩ2
Δt
πΔt
Δt
ΔtTp
H(Ω)
H(Ω)
h(t)
G(Ω) =ˆ t1
0e−iΩtdt =
sin(Ωt1)Ω
+ icos(Ωt1) − 1
Ω
ΔΩ
NΔΩN ΔΩ
2
N2
N2
g(mΔt) =12π
N−1∑n=0
G(nΔΩ)e2πim nN ΔΩ
N = 16 ΔΩ = 1,25π.
N ΔΩ2
N
H(Ω) =1
m(ω2 − Ω2)
ωh(t)
H(Ω)
ΔΩ = 0,15625Tp = 64 × 0,15625 = 10
H(nΔΩ)
H(nΔΩ) =1
m(ω2 − Ω2)
H(Ω).
g(mΔt) =12π
N−1∑n=0
G(nΔΩ)e2πim nN ΔΩ
h(mΔt) =12π
N−1∑n=0
H(nΔΩ)e2πim nN ΔΩ
H(Ω)h(t)
h(t) =1
mΩsin(Ωt) t > 00 t < 0
h(t)
h
H(Ω) h(t)
h(t)”ξ”
h(t)
ΔΩ
Tp = 2πΔΩ
h(t) 2πrΔΩ r
−∞ ∞
h(t) =1
mωde−ξω(t− 2π
ΔΩm)sinωd(t− 2π
ΔΩm)
m
h(t)
h(t)
h(t) =1
mωd
0∑r=−∞
e−ξω(t−rTp)sin(ωd(t − rTp))
sinθ = 12(eiθ − e−iθ)
h(t) =1
mωde−ξωt
0∑r=−∞
eξωrTpeiωd(t−rTp) − e−iωd(t−rTp)
2i=
=1
mωd
e−ξωt
2i
{eiωdt
0∑r=−∞
e−rTp(−ξω+iωd) − e−iωdt0∑
r=−∞e−rTp(−ξω−iωd)
}
−r r
h(t) =1
mωd
e−ξωt
2i
{eiωdt
∞∑r=0
erTp(−ξω+iωd) − e−iωdt∞∑
r=0
erTp(−ξω−iωd)
}
h(t) =1
mωd
e−ξωt
2i
{eiωdt
1 − eTp(−ξω+iωd)− e−iωdt
1 − eTp(−ξω−iωd)
}
h(t) =e−ξωt
mωd
{sin(ωdt) − e−ξωTpsin(ωd(t − Tp)1 − 2e−ξωTpcos(ωdTp) + e−2ξωTp
}
h(t) h(t)Tp Tp h(t)
h(t)
Tp
ξ = 0
h(t) =1
2mω(sin(ωt) +
cos(ωt)sin(ωTp)1 − cos(ωTp)
h(t)
h(t) h(t) Tp
h(t)
g(t) Tp
h
Th,
h
g h
Tp = pΔt Th = qΔt T0 T0 = NΔt = (p + q + 1)Δt
Th
Th
Th
h
Th
Tp +Th
g tp
g
tpTh g
g
′t′p
th
g Tp
Tp
T0 = Tp + T2
T0.
h(t),0 < t < T0
t = 0,−T0,−2T0... h(t)
h(t) =e−ξωt
mωd
{sin(ωdt) − e−ξωT0sin(ωd(t − T0))1 − 2e−ξωT0cos(ωdT0) + e−2ξωT0
}
u(kΔt)g(t)
u(mΔt) =N−1∑j=0
g(jΔt)h {(m − j)Δt}Δt
u(mΔt) =12π
N−1∑n=0
G(nΔΩ)H(nΔΩ)e2πim nN ΔΩ
G(nΔΩ) g(mΔt) H(nΔΩ)h(mΔt)
u(mΔt) u(mΔt)
t = 0 u(mΔt) u(mΔt)0 < t < T0
T0
u(mΔt)
u(mΔt)u(mΔt)
t = 0 u(0) u(0)
u(mΔt) u(0)t = 0 u(0)
u(0) u(0)
t = 0 u(0)
u(mΔt) =12π
N−1∑n=0
G(nΔΩ)H(nΔΩ)e2πim nN ΔΩ
H(nΔΩ) h(t)
h(t) =1
mωd
e−ξωt
2i
{eiωdt
1 − eT0(−ξω+iωd)− e−iωdt
1 − eT0(−ξω−iωd)
}
U(Ω).
U(Ω).
U(nΔΩ) = G(nΔΩ)H(nΔΩ)
U(nΔΩ)−N
2N2 ,
u(mΔt) =1T0
N2∑
n=−N2
U(nΔΩ)e2πin tT0
t = mΔt
T0 = NΔt
ΔΩ = 2πT0
t = 0 t = 0
u(0) =2πi
T 20
N2∑
n=−N2
nU(nΔΩ) =2πi
T 20
N2∑
n=−N2
nRe {U(nΔΩ)} + inIm {U(nΔΩ)}
Re {U(nΔΩ)} ⇒ U(nΔΩ)Im {U(nΔΩ)} ⇒ U(nΔΩ)
Re {U(nΔΩ)} nRe {U(nΔΩ)}
Im {U(nΔΩ)} nIm {U(nΔΩ)}
u(0) =−4π
T 20
N2∑
n=0
nIm {U(nΔΩ)}
Δu(0) = u(0) − u(0)
Δu(0) = u(0) − u(0)
u(kΔt)Δu(0) Δu(0)
t = 0
r(t) = e−ξωt(cos(ωdt) +ξω
ωdsin(ωdt))
t = 0
s(t) =e−ξωt
ωdsin(ωdt)
η1(t) = Δu(0)r(t)
η2(t) = Δu(0)s(t)
u(mΔt) = u(mΔt) + η1(mΔt) + η2(mΔt)
δ(t) N − 2u1 δ(t) N − 1
u2
δ(t) u1 h (N−2)Δtu2 h (N − 1)Δt
R1 R2
u(mΔt) = u(mΔt) + R1u1(mΔt) + R2u2(mΔt)
R1u1(0) + R2u2(0) = u(0) − u(0)R1 ˙u1(0) + R2 ˙u2(0) = u(0) − ˙u(0)
u(0) u(0)
u(0)
u(mΔt) =12π
N−1∑n=0
G(nΔΩ)H(nΔΩ)e2πim nN ΔΩ
˙u(0)
˙u(0) = − 4π
(T0)2
N2∑
n=0
nIm {U(nΔΩ)}
˙u1(0) ˙u2(0) h(t)
˙h(t) =1
mωdΔe−ξωt
{ωdcosωdt − ωde
−ξωT0cosωd(t − T0)}− ξωh(t)
Δ = 1 − 2e−ξωT0cosωdT0 + e−2ξωT0
˙u1(t) ˙h(t) (N − 2)Δt
˙u2(t) ˙h(t) (N−1)Δt
u1(0) = h(2Δt) ˙u1(0) = ˙h(2Δt)u2(0) = h(Δt) ˙u2(0) = ˙h(Δt)
R1 R2
u(nΔt) =N−1∑n=0
g(nΔt)h {(m − n)Δt}Δt
G(nΔΩ) =N−1∑m=0
g(mΔt)e−2πin mN Δt
G(nΔΩ) g(t).
H(nΔΩ) =N−1∑k=0
h(kΔt)e−2Πin kN Δt
H(nΔΩ)h(t).
U(nΔΩ) = G(nΔΩ)H(nΔΩ)
U(nΔΩ)
u(mΔt) =12π
N−1∑n=0
U(nΔΩ)e2πin mN
u(mΔt)
N2
N2
N2
N = 2γ γ
X(n) =N−1∑m=0
x(m)e−2πin mN
Δt.γ = 3.
W = e−2π iN
n m
n = 4n2 + 2n1 + n0
m = 4m2 + 2m1 + m0
n0 n1 n2 m0 m1 m2
X(n2, n1, n0) =1∑
m0=0
1∑m1=0
1∑m2=0
x(m2, m1, m0)Wnm
Wnm
Wnm = W (4n2+2n1+n0)(4m2+2m1+m0) = W (4n2+2n1+n0)4m2W (4n2+2n1+n0)2m1W (4n2+2n1+n0)m0
WmN = e−2πim NN = cos(2mπ) − isin(2mπ) = 1
W 16n2m2 = W 8n1m2 = W 8n2m1 = 1
Wnm = W 4n0m2W (2n1+n0)2m1W (4n2+2n1+n0)m0
X(n2, n1, n0) =1∑
m0=0
1∑m1=0
{1∑
m2=0
x(m2, m1, m0)W 4n0m2
}W (2n1+n0)2m1W (4n2+2n1+n0)m0
x1(n0, m1, m0) =1∑
m2=0
x(m2, m1, m0)W 4n0m2
m1 m0 n0
x1(n0, m1, m0) = x(0, m1, m0)W 0 + x(1, m1, m0)W 4n0
x1 xn0 = 1 m1 = 0 m0 = 1
x1(1, 0, 1) = x1(5) =
x(0, 0, 1)W 4×1×0 + x(1, 0, 1)W 4×1×1 = x(1) + x(5)
x x1
x(1) x(5) W 4
x(5) x1(5)4n0m2 m2 = 0 4n0 m2 = 1
W 4n0 , n0 = 0,W 0
x x1
(N − 1)x1
x1(0) x1(4)
x1(0) = x(0) + x(4)W 0
x1(4) = x(0) + x(4)W 4
x1
m1 m0 n0 = m2 = 0n0 = m2 = 1. N
2 = 4W s W s+(N
2)
W s+(N2
) = e(2π iN
)(N2
+s) = eiπe2iπ sN = −W s
x1(j) = x(j) + x(N2 + j)W s
x1(N2 + j) = x(j) − x(N
2 + j)W s
x x1N2
x2(n0, n1, m0) =1∑
m1=0
x1(n0, m1, m0)W (2n1+n0)2m1
n0 n1 m0 x2(n0, n1, m0)x2 x1
W (2n1+n0)2m1
x1 x2N2 N − 1
x3(n0, n1, n2) =1∑
m0=0
x2(n0, n1, m0)W (4n2+2n1+n0)m0
X x3
X(n2, n1, n0) = x3(n0, n1, n2)
X
X x3
x1 x2 x3
γ = log2NN2 (N
2 )log2N.
m = 0,25
t1 = 0,6
ξ = 0,06.
π2
ω = 2π
p = sin( 21,2 t)
ωd = ω√
1 − ξ2
mu + cu + ku = p(t)
mu + cu + ku = 0
u = e−ωξt[C1sinωdt + C2cosωdt] +p0
k
(1 − (Ωω )2)sinΩt − 2ξ Ω
ω cosΩt
[1 − (Ωω )2]2 + 4ξ2(Ω
ω )2
C1 C2
−0,2423 0,097
u = e−0,377t − 0,2423sin(6,2718t) + e−0,377t0,097cos(6,2718t) + 0,299sin(5,235t) − 0,097cos(5,235t).
u = e−0,377t(−0,040sin(6,2718t) + 0,1475cos(6,2718t).
t
2,9s0,1s
t u t u
2,9s
¯h(t) g(t)H(Ω)
G(Ω)U(Ω) u(t)
t u u t u u
2,9h(t)
h(t)
5s
h(t) 10s
30s
15s
h(t)
u(mΔt) = u(mΔt) + η1(mΔt) + η2(mΔt)
η1 μ2
2,9
t u u u t u u u
{u}φn(t)
{u} =M∑
n=1
φnyn
[φ]M n M
n
yn + 2ξnωnyn + ω2nyn = pn
y0n = φTnMu0
y0n = φTnMv0
n
M ¨{u} + C{u} + K{u} = fg(t)
f
g(t)
H(Ω)eiΩt
{u} = HeiΩt
(−Ω2M + iΩC + K)H = f
Ω HHR + iHI 2N
N
Ω H 2N
Hj j
(u)G × Hj, G
g(t)
uj(mΔt) =12π
L−1∑l=0
Hj(lΔΩ)G(lΔΩ)e2πim lL ΔΩ
LΔtΔt
uj G(lΔΩ)uj
uj uj
Hj Hj
Hj Hj
Hj(Ω) =∞∑
s=−∞Hj(Ω + s
2π
Δt)
s 2πΔt Hj(Ω)
H(Ω)
πΔt
Hj(Ω) Ω � πΔt Hj(Ω) � Hj
Hj(Ω)
uj(mΔt) =12π
L−1∑l=0
Hj(lΔΩ)G(lΔΩ)e2πim lL ΔΩ
Rp tpT0
Rp
up(tp) = Rphj(tp)
hj Hj
hj =12π
L−1∑l=0
Hj(lΔΩ)ΔΩ
uj(0) = uj(0) +2N∑p=1
Rphj(tp)
2N∑p=1
Rphj(tp) = uj(0) − uj(0)
2N∑p=1
Rp˙hj(tp) = uj(0) − ˙uj(0)
uj(mΔt) = uj(mΔt) +2N∑p=1
Rphj(tp + mΔt)
hj(t)˙hj(t)
hj Hj(lΔΩ)˙hj(t)
p
˙hj(tp) =hj(tp + Δt) − hj(tp − Δt)
2Δt
h(t)
(p1
p2
)=
(1,000,75
)p
m2 = 2 m1 = 3
k1 = 100 k2 = 150
t1 = 1,00
ξ = 0,00.
p = 20
Δt = 0,05
t
M {u} + K {u} = {p(t)}
i
yi + ω2i yi = pi
K =(
250 −100−100 100
)M =
(3 00 2
)
|K − ω2i M | = 0
ω1 = 4,75rad/s ω2 = 10,52rad/s
(K − ωiM) {ai} = 0
a1 =(
1,001,82
)a2 =
(1,00−0,82
)
y1 + ω21y1 = p1
y2 + ω22y2 = p2
ω1 = 4,75 ω2 = 10,52
hi(t) =1
2Miωi(sinωit +
cosωitsinωiT0
1 − cosωiT0)
Mi i Mi = {ai}T M {ai}
t y y y t y y y
T0 = 3s.
(−Ω2M + K)H = f
f
f =(
10,75
)M K f
H
[250 − 3Ω2 −100
−100 100 − 2Ω2
]H =
(1
0,75
)
H(Ω)H(Ω) Ω
Δt = 0,05s.
ΔΩ = 2πT0
= 2,09N2 ΔΩ = 60
2 2,09 = 62,70rad/s
H(Ω)
H(Ω) H1(Ω) H2(Ω)
H1 (Ω) � H1(Ω) H2 (Ω) � H2(Ω)
H1(Ω) H2(Ω)g(kΔt)
G(kΔΩ)
{U(kΔΩ)} = {G(kΔΩ)}(
H1(kΔΩ)H2(kΔΩ)
)
R1h1(0,40) + R2h1(0,30) + R3h1(0,40) + R4h1(0,40) = u1(0)
R1h2(0,40) + R2h2(0,30) + R3h2(0,40) + R4h2(0,40) = u2(0)
R1˙h1(0.40) + R2
˙h1(0.30) + R3˙h1(0.20) + R4
˙h1(0.40) = ˙u1(0)
R1˙h2(0.40) + R2
˙h2(0.30) + R3˙h2(0.20) + R4
˙h2(0.40) = ˙u2(0)
u1(0) = −0,049 u2(0) = 0,084 ˙u1(0) = 2,8228 ˙u2(0) = 0,463.
R1 R2 R3 R4
R1 = 458,952 R2 = −972,150 R3 = 994,566 R4 = −444,381
uj(mΔt) = uj(mΔt) +2N∑p=1
Rphj(tp + mΔt)
fn1 =π
2
√EaI
mL4
Ea
I
m
L
Rx(τ)
Rx(τ)
DEP (Ω) =12π
ˆ +∞
−∞Rx(τ)e−iΩτdτ
Rx(τ) =ˆ +∞
−∞DEP (Ω)eiΩτdΩ
m
αβ α β
DEP =1
2πΔfA(Ω)A∗(Ω)
ΔfA(Ω) a(t)
A∗(Ω) A(Ω)
Ea = 210000 Nmm2
Ixx = 450,10−8m4
m = 20,4kgm
±30g.
N = 26322400Hz
2400
1200Hz.
DEP =1
2πΔfA(Ω)A∗(Ω)
357,4Hz
fn1 =π
2
√EaI
mL4
fn1 =π
2
√2,1E11 × 450E−8
20,4 × 0,904= 417,39Hz
R = ku R u
ξ =δ√
4π2 + δ2
δ
(ti, ai),
yi = L(ai).
τi = tif f
(τi, yi)
y = aτ + b
δ = −a
δ.
δ = 0,070ξ = 0,070√
4π2+0,0702= 0,070
6,283 = 0,011 ξ = 1,1 %