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ESERCIZI TSB 2
2 D
D λ=
=
z m 4 z
4 λ m
c
=
f
λ R × Ru
1
=R
R × R × R = =300
R Ω
1 4 3 2 2 R 3
( )
( )
=R −T
R 1+ a T 0
t 0 R1’=
( )
( )
−T =158.4
R 1+ a T 0 Ω
1
R1’ = R1 dopo l’aumento di
temperatura Δ R
A 1
⋅
=V =0.112
V ¿
0 2 R
( )
1+ A 1
R R
2 4
=
A=
Con R R 3
1 √
− 3
( )=1 ( )=
ϑ ϑ
=kH
V cos cos
I 2
( ) ( )−kH ( ) ( )=0
ϑ ϑ
=KH
V cos 60 cos sin 60 sin
II √
−1 3
( )
+V =
aVR= V I II
2 4
PER RICAVARE VII USO SEMPRE L’ANGOLO 60
PER RICAVARE VIII USO SEMPRE L’ANGOLO 120 −t −t /
T T
( ) ( ) ( )
ⅇ ⅇ
=M =M
M t 0 sen a
2 2
xy xy 0
c G = zm/F zm
−4
=4.4
λ= ×10
f z m =gF=200
z
= g*F g= m
F
2
D
=
z m 4 λ
√
D= z 4 λ=18,7616
m
λF
= =0.125
W D
=R
R × R × R
1 4 2 3
R × R
1 4
= =400
R Ω
2 R 3
ⅆ ⅆ
R l
=
G= R l
ⅆ ⅆ
R l
=G =0.1 Ω
R l ⅆ
A R
⋅
=V =0.32V
V ¿ R
2
( )
1+ A
R R
2 4
= =4
A= R R
1 3
1 zp c
=2 =110
zp= mm
F c 2 f
R c c
zp ≥ f≤
2 f 2 zp
C
=
f
- con zp in metri
MAx 2 zp 2
c D
λ= =
z m
f 4 λ
2 d
t= d = t*c/2
c ( )
π
( )=M =1
=1 M
Mxy 0 sen 0
0 2
1 1
−t ∕ T 2
( ) ( ) ⅇ
=Mxy =1⋅ = =0.169
Mxy t 0 t ∕ T 80 ∕ 45
ⅇ ⅇ
2
−t 1
( )
−t ∕ T T
( )=M ( ) ⅇ =0,28346
+ =1−
M t 1−ⅇ Mz 0
1 1
z 0 80 ∕ 240
ⅇ
( ) ( )
Mxy 0.109 0
=atan =atan =30
α Mz 0.710 ϑ
=kH
V cos
I √
1 3
ϑ− ϑ
=
V kH cos kH sin
II 2 2
v √
1 3
II = − tanϑ
v 2 2
I ( ) ( )
v 2 v
−2 1 1
II II
ϑ= − =
tan 1−
√ √
v 2 v
3 3
I I
( )
( )
2 v
1 II
ϑ=atan 1−
√ v
3 I