Gra ci
Legenda:
S11 - spettro della componente uttuante longitudinale u
S22 - spettro della componente uttuante trasversale v
S33 - spettro della componente uttuante verticale w
Negli spettri adimensionali (rappresentazione di Kaimal) vale quella allegata:
C.1. Sonda 55P61 - (2C) - Condizione di prova Re
θ
1 10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027369 [−], z =0.008 [m]
S11
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.032843 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.039685 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.048922 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.060896 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.076976 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.097503 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12487 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16079 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.20766 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.26924 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.34998 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.45604 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.59528 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.77797 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0174 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.3322 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7448 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2511 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.7643 [−], z =0.808 [m]
Figura C.1.: Densità spettrali di potenza del segnale originale - Sonda 55P61 - 2C - Condizione di prova Re
θ110−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100
f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027369 [−], z =0.008 [m]
S11
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.032843 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.039685 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.048922 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.060896 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.076976 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.097503 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12487 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16079 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.20766 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.26924 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.34998 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.45604 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.59528 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.77797 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0174 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.3322 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7448 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2511 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.7643 [−], z =0.808 [m]
Figura C.2.: Densità spettrali di potenza del segnale elaborato - Sonda 55P61 - 2C - Condizione di prova Re
θ110−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2
f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.027369 [−], z =0.008 [m]
u
w
uw
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.032843 [−], z =0.0096 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.039685 [−], z =0.0116 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.048922 [−], z =0.0143 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.060896 [−], z =0.0178 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.076976 [−], z =0.0225 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.097503 [−], z =0.0285 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.12487 [−], z =0.0365 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.16079 [−], z =0.047 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.20766 [−], z =0.0607 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.26924 [−], z =0.0787 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.34998 [−], z =0.1023 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.45604 [−], z =0.1333 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.59528 [−], z =0.174 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.77797 [−], z =0.2274 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.0174 [−], z =0.2974 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.3322 [−], z =0.3894 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.7448 [−], z =0.51 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.2511 [−], z =0.658 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.7643 [−], z =0.808 [m]
Figura C.3.: Densità spettrali di potenza adimensionali - Sonda 55P61 - 2C - Condizione di prova Re
θ1C.2. Sonda 55P61 - (2C) - Condizione di prova Re
θ
2 10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.02885 [−], z =0.008 [m]
S11
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.03462 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.041832 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.051569 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.06419 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.08114 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.10278 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.13163 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16949 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.2189 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.28381 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.36891 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.48071 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.62748 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.82005 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0725 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.4043 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.8392 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.3729 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.9138 [−], z =0.808 [m]
Figura C.4.: Densità spettrali di potenza del segnale originale - Sonda 55P61 - 2C - Condizione di prova Re
θ210−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100
f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.02885 [−], z =0.008 [m]
S11
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.03462 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.041832 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.051569 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.06419 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.08114 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.10278 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.13163 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16949 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.2189 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.28381 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.36891 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.48071 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.62748 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.82005 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0725 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.4043 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.8392 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.3729 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.9138 [−], z =0.808 [m]
Figura C.5.: Densità spettrali di potenza del segnale elaborato - Sonda 55P61 - 2C - Condizione di prova Re
θ210−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2
f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.02885 [−], z =0.008 [m]
u
w
uw
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.03462 [−], z =0.0096 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.041832 [−], z =0.0116 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.051569 [−], z =0.0143 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.06419 [−], z =0.0178 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.08114 [−], z =0.0225 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.10278 [−], z =0.0285 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.13163 [−], z =0.0365 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.16949 [−], z =0.047 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.2189 [−], z =0.0607 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.28381 [−], z =0.0787 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.36891 [−], z =0.1023 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.48071 [−], z =0.1333 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.62748 [−], z =0.174 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.82005 [−], z =0.2274 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.0725 [−], z =0.2974 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.4043 [−], z =0.3894 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.8392 [−], z =0.51 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.3729 [−], z =0.658 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.9138 [−], z =0.808 [m]
Figura C.6.: Densità spettrali di potenza adimensionali - Sonda 55P61 - 2C - Condizione di prova Re
θ2C.3. Sonda 55P91 - (3C-co) - Condizione di prova Re
θ
1 10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027653 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.033184 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.040097 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.04943 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.061528 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.077774 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.098514 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12617 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16246 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.20982 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.27204 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.35361 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.46077 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.60145 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.78604 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.028 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.346 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7629 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2745 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.7929 [−], z =0.808 [m]
Figura C.7.: Densità spettrali di potenza del segnale originale - Sonda 55P91 - 3C-co - Condizione di prova Re
θ110−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100
f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027653 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.033184 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.040097 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.04943 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.061528 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.077774 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.098514 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12617 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16246 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.20982 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.27204 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.35361 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.46077 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.60145 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.78604 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.028 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.346 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7629 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2745 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.7929 [−], z =0.808 [m]
Figura C.8.: Densità spettrali di potenza del segnale elaborato - Sonda 55P91 - 3C-co - Condizione di prova Re
θ110
−310
−210
−110
010
110
2−0.5
0
0.5
1
1.5
2
f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.027653 [−], z =0.008 [m]
u
v
w
uw
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.033184 [−], z =0.0096 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.040097 [−], z =0.0116 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.04943 [−], z =0.0143 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.061528 [−], z =0.0178 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.077774 [−], z =0.0225 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.098514 [−], z =0.0285 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.12617 [−], z =0.0365 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.16246 [−], z =0.047 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.20982 [−], z =0.0607 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.27204 [−], z =0.0787 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.35361 [−], z =0.1023 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.46077 [−], z =0.1333 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.60145 [−], z =0.174 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.78604 [−], z =0.2274 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.028 [−], z =0.2974 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.346 [−], z =0.3894 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.7629 [−], z =0.51 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.2745 [−], z =0.658 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.7929 [−], z =0.808 [m]
Figura C.9.: Densità spettrali di potenza adimensionali - Sonda 55P91 - 3C-co - Condizione di prova Re
θ1C.4. Sonda 55P91 - (3C-co) - Condizione di prova Re
θ
210
−410
−310
−210
−110
010
110
210
310
410
−810
−610
−410
−210
0f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.029165 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.034998 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.042289 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.052133 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.064892 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.082027 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.1039 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.13307 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.17135 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.22129 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.28691 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.37295 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.48596 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.63434 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.82902 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0842 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.4196 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.8593 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.3988 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.9457 [−], z =0.808 [m]
Figura C.10.: Densità spettrali di potenza del segnale originale - Sonda 55P91 - 3C-co - Condizione di prova Re
θ210−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100
f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.029165 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.034998 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.042289 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.052133 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.064892 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.082027 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.1039 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.13307 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.17135 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.22129 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.28691 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.37295 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.48596 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.63434 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.82902 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0842 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.4196 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.8593 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.3988 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.9457 [−], z =0.808 [m]
Figura C.11.: Densità spettrali di potenza del segnale elaborato - Sonda 55P91 - 3C-co - Condizione di prova Re
θ210−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2
f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.029165 [−], z =0.008 [m]
u
v
w
uw
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.034998 [−], z =0.0096 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.042289 [−], z =0.0116 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.052133 [−], z =0.0143 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.064892 [−], z =0.0178 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.082027 [−], z =0.0225 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.1039 [−], z =0.0285 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.13307 [−], z =0.0365 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.17135 [−], z =0.047 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.22129 [−], z =0.0607 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.28691 [−], z =0.0787 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.37295 [−], z =0.1023 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.48596 [−], z =0.1333 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.63434 [−], z =0.174 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=0.82902 [−], z =0.2274 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.0842 [−], z =0.2974 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.4196 [−], z =0.3894 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=1.8593 [−], z =0.51 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.3988 [−], z =0.658 [m]
10−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2f · z /U [-]
f
·
S
ij/
u
2 ∗[-]
z/
δ
=2.9457 [−], z =0.808 [m]
Figura C.12.: Densità spettrali di potenza adimensionali - Sonda 55P91 - 3C-co - Condizione di prova Re
θ2C.5. Sonda 55P91 - (3C) - Condizione di prova Re
θ
1 10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027845 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.033415 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.040376 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.049774 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.061956 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.078315 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.099199 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12704 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16359 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.21128 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.27393 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.35607 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.46397 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.60564 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.79151 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.0352 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.3554 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7751 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2903 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.8124 [−], z =0.808 [m]
Figura C.13.: Densità spettrali di potenza del segnale originale - Sonda 55P91 - 3C - Condizione di prova Re
θ110−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100
f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.027653 [−], z =0.008 [m]
S11
S22
S33
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.033184 [−], z =0.0096 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.040097 [−], z =0.0116 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.04943 [−], z =0.0143 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.061528 [−], z =0.0178 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.077774 [−], z =0.0225 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.098514 [−], z =0.0285 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.12617 [−], z =0.0365 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.16246 [−], z =0.047 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.20982 [−], z =0.0607 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.27204 [−], z =0.0787 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.35361 [−], z =0.1023 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.46077 [−], z =0.1333 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.60145 [−], z =0.174 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=0.78604 [−], z =0.2274 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.028 [−], z =0.2974 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.346 [−], z =0.3894 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=1.7629 [−], z =0.51 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.2745 [−], z =0.658 [m]
10−410−310−210−1100101102103104 10−8 10−6 10−4 10−2 100f
[Hz]
S
ii[m
2s
2/
H
z]
z/
δ
=2.7929 [−], z =0.808 [m]
Figura C.14.: Densità spettrali di potenza del segnale elaborato - Sonda 55P91 - 3C - Condizione di prova Re
θ110−3 10−2 10−1 100 101 102 −0.5 0 0.5 1 1.5 2
