Two Port Networks

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Two Port Networks
1. Two Two-port networks are connected in cascade. The combination is to the represented
as a single two – port network, by multiplying the individual
(a) z-parameter matrices
(c) y-parameter matrices
(b) h-parameter matrices
(d) ABCD parameter
[GATE 1991: 2 Marks]
Soln. ABCD parameters relate the voltage and current at one port to voltage and current
at the other port
Option (d)
2. For a 2-port network to be reciprocal,
(a) z11 = z22
(b) y21 = y12
Soln.
(c) h21 = -h12
(d) AD – BC = 0
[GATE 1992: 2 Marks]
π’šπŸπŸ = π’šπŸπŸ
π’‰πŸ = −π’‰πŸπŸ
Option (b) & (c)
3. The condition, that a 2-port network is reciprocal, can be expressed in terms of its ABCD
parameters as…….
[GATE 1994: 1 Mark]
Soln. AD – BC = 1
4. In the circuit of figure, the equivalent impedance seen across terminals A, B is
A
2
4
j2
Zeq
a
b
-j 2
2
4
B
(a) (16/3) Ω
(b) (8/3) Ω
(c) (8/3 + 12j) Ω
(d) None of the above
[GATE 1997: 2 Marks]
Soln. The product of the opposite arms are equal, so the bridge is balanced.
The point a and b are at the same potential
𝒁𝒆𝒒 = (πŸβ€–πŸ’) + (πŸβ€–πŸ’)
=
πŸ’ πŸ’ πŸ–
+ =
πŸ‘ πŸ‘ πŸ‘
Option (b)
5. The short-circuit admittance matrix of a two-port network is
0 −1⁄2
[
]
1⁄
0
2
The two – port network is
(a) non – reciprocal and passive
(c) reciprocal and passive
(b) non – reciprocal and active
(d) reciprocal and active
[GATE 1998: 1 Marks]
Soln.
π’šπŸπŸ ≠ π’šπŸπŸ
so the network is nonreciprocal. And active networks are
nonreciprocal
Option (b)
6. A 2-port network is shown in the figure. The parameter h21 for this network can be given
by
I1
I2
+
+
R
V1
R
R
V2
-
(a) -1/2
(b) +1/2
(c) -3/2
(d) +3/2
[GATE 1999: 1 Mark]
Soln.
π‘½πŸ = π’‰πŸπŸ π‘°πŸ + π’‰πŸπŸ π‘½πŸ
π‘°πŸ = π’‰πŸπŸ π‘°πŸ + π’‰πŸπŸ π‘½πŸ
π’‰πŸπŸ =
π‘°πŸ
|
π‘°πŸ π‘½πŸ=𝟎
π‘½πŸ = π‘Ήπ‘°πŸ + 𝑹(π‘°πŸ + π‘°πŸ )
Or πŸπ‘Ήπ‘°πŸ + π‘Ήπ‘°πŸ = π‘½πŸ
When π‘½πŸ = 𝟎, πŸπ‘Ήπ‘°πŸ + π‘Ήπ‘°πŸ = 𝟎
So,
π‘°πŸ
π‘°πŸ
=
−𝑹
πŸπ‘Ή
Option (a)
=−
𝟏
𝟐
7. The admittance parameter Y12 in the 2-port network in figure is
I1
E1
20
I2
5
(a) -0.2 nho
(b) 0.1 mho
Soln.
π’šπŸπŸ = −
E2
5
(c) -0.05 mho
(d) 0.05 mho
[GATE 2001: 1 Mark]
𝟏
𝟐𝟎
= −𝟎. πŸŽπŸ“ π’Žπ’‰π’π’”
Option (c)
8. The Z parameters Z11 and Z21 for the 2-port network in the figure are
I1
I2
2
4
E2
E1
10E1
(a) 𝑍11 =
−6
16
Ω, 𝑍21 = 11 Ω
11
6
4
(b) 𝑍11 = 11 Ω, 𝑍21 = 11 Ω
6
−16
4
11
4
(c) 𝑍11 = 11 Ω, 𝑍21 =
Ω
(d) 𝑍11 = 11 Ω, 𝑍21 = 11 Ω
[GATE 2001: 2 Marks]
Soln. For z – parameters
π‘¬πŸ = π’πŸπŸ π‘°πŸ + π’πŸπŸ π‘°πŸ
π‘¬πŸ = π’πŸπŸ π‘°πŸ + π’πŸπŸ π‘°πŸ
Writing KVL in LHS loop
π‘¬πŸ = πŸπ‘°πŸ + πŸ’π‘°πŸ + πŸ’π‘°πŸ − πŸπŸŽπ‘¬πŸ
Or
πŸπŸπ‘¬πŸ = πŸ”π‘°πŸ + πŸ’π‘°πŸ − − − −(𝑰)
π’πŸπŸ =
π’πŸπŸ =
π‘¬πŸ
π‘°πŸ
π‘¬πŸ
π‘°πŸ
|π‘°πŸ=𝟎 =
|π‘°πŸ=𝟎 =
πŸ”
𝟏𝟏
πŸ’
𝟏𝟏
Ω
Ω
Writing KVL in RHS Loop
π‘¬πŸ = πŸ’(π‘°πŸ + π‘°πŸ ) − πŸπŸŽπ‘¬πŸ − − − − − (𝑰𝑰)
πŸ”π‘°πŸ +πŸ’π‘°πŸ
Substituting π‘¬πŸ =
𝟏𝟏
π‘¬πŸ = πŸ’(π‘°πŸ + π‘°πŸ ) −
π’πŸπŸ =
π‘¬πŸ
π‘°πŸ
|π‘°πŸ=𝟎 =
π’Šπ’ π’†π’’π’–π’‚π’•π’Šπ’π’ − −(𝑰𝑰𝑰)
𝟏𝟎(πŸ”π‘°πŸ +πŸ’π‘°πŸ )
−πŸπŸ”
𝟏𝟏
𝟏𝟏
Ω
Option (c)
9. The impedance parameters Z11 and Z12 of the two-port network in the figure are
2
2
2
1
2
1
1
(a) 𝑍11 = 2.75Ω π‘Žπ‘›π‘‘ 𝑍12 = 0.25 Ω
(b) 𝑍11 = 3 Ω π‘Žπ‘›π‘‘ 𝑍12 = 0.5Ω
1
2
(c) 𝑍11 = 3 Ω π‘Žπ‘›π‘‘ 𝑍12 = 0.25Ω
(d) 𝑍11 = 2.25Ω π‘Žπ‘›π‘‘ 𝑍12 = 0.5 Ω
[GATE 2003: 2 Marks]
Soln. Using βˆ† − 𝒀 conversion, the circuit reduces to
2
0.5
0.5
Z1
2
Z2
Z3
0.25
π’πŸπŸ = π’πŸ + π’πŸ‘
= 𝟐. πŸ“ + 𝟎. πŸπŸ“
= 𝟐. πŸ•πŸ“β„¦
π’πŸπŸ = π’πŸ‘ = 𝟎. πŸπŸ“β„¦
Option (a)
10. The h parameter of the circuit shown in the figure are
I1
I2
10
+
V1
0.1 0.1
]
−0.1 0.3
10 −1
(b) [
]
1 0.05
(a) [
+
20
V2
30 20
]
20 30
10
1
(d) [
]
−1 0.05
[GATE 2005: 2 Marks]
(c) [
Soln.
π‘½πŸ = π’‰πŸπŸ π‘°πŸ + π’‰πŸπŸ π‘½πŸ
π‘°πŸ = π’‰πŸπŸ π‘°πŸ + π’‰πŸπŸ π‘½πŸ
Writing KVL in LHS and RHS Loop
π‘½πŸ = πŸπŸŽπ‘°πŸ + 𝟐𝟎(π‘°πŸ + π‘°πŸ ) − − − − − −(π’Š)
π‘½πŸ = 𝟐𝟎(π‘°πŸ + π‘°πŸ ) − − − − − −(π’Šπ’Š)
Or π‘½πŸ = πŸπŸŽπ‘°πŸ + π‘½πŸ
π’‰πŸπŸ =
π’‰πŸπŸ =
π’‰πŸπŸ =
π’‰πŸπŸ =
π‘½πŸ
|
π‘°πŸ π‘½πŸ =𝟎
π‘°πŸ
|
π‘°πŸ π‘½πŸ =𝟎
π‘½πŸ
|
π‘½πŸ π‘°πŸ =𝟎
π‘°πŸ
π‘½πŸ
= 𝟏𝟎
= −𝟏
=𝟏
|π‘°πŸ=𝟎 =
𝟏
𝟐𝟎
= 𝟎. πŸŽπŸ“β„¦
Option (d)
11. In the two network shown in the figure below Z12 and Z21 are, respectively
I1
I2
βI1
re
(a) π‘Ÿπ‘’ π‘Žπ‘›π‘‘ π›½π‘Ÿ0
(b) 0 π‘Žπ‘›π‘‘ − π›½π‘Ÿ0
r0
(c) 0 π‘Žπ‘›π‘‘ π›½π‘Ÿ0
(d) π‘Ÿπ‘’ π‘Žπ‘›π‘‘ −π›½π‘Ÿ0
[GATE 2006: 1 Mark]
Soln.
I1
I2
re
V1
βI1
r0
π‘½πŸ = π’πŸπŸ π‘°πŸ + π’πŸπŸ π‘°πŸ
π‘½πŸ = π’πŸπŸ π‘°πŸ + π’πŸπŸ π‘°πŸ
π’πŸπŸ =
π‘½πŸ
|
π‘°πŸ π‘°πŸ =𝟎
When π‘°πŸ = 𝟎, π‘½πŸ = 𝟎,
π’πŸπŸ =
𝒔𝒐
π‘½πŸ
|
π‘°πŸ π‘½πŸ =𝟎
When π‘°πŸ = 𝟎, π‘½πŸ = −πœ·π‘°πŸ π’“πŸŽ
π’πŸπŸ = −πœ·π’“πŸŽ
Option (b)
π’πŸπŸ = 𝟎
V2
12. For the two-port network shown, the short-circuit admittance parameter matrix is
0.5
1
2
yb
yc
ya
0.5
0.5
1
4 −2
]𝑆
−2 4
1
−0.5
(b) [
]𝑆
−0.5
4
1 −0.5
]𝑆
0.5
1
4 2
(d) [
]𝑆
2 4
[GATE 2010: 1 Mark]
(a) [
(c) [
Soln. The short circuit admittance parameters of a two port π network:
π’šπŸπŸ = π’šπ’‚ + π’šπ’ƒ =
𝟏
𝟎.πŸ“
+
π’šπŸπŸ = π’šπŸπŸ = −π’šπ’ƒ = −
π’šπŸπŸ = π’šπ’ƒ + π’šπ’„ =
𝟏
𝟎.πŸ“
+
𝟏
= πŸ’β„¦
𝟎.πŸ“
𝟏
𝟎.πŸ“
𝟏
𝟎.πŸ“
= −πŸβ„¦
= πŸ’β„¦
Option (a)
13. If the scattering matrix [S] of a two port network is
0
0
[𝑆] = [0.2∠00 0.9∠00 ]
0.9∠0 0.1∠0
Then the network is
(a) Lossless and reciprocal
(c) Not lossless but reciprocal
(b) Lossless but not reciprocal
(d) Neither lossless not reciprocal
[GATE 2010: 1 Mark]
Soln. For the reciprocal network |π‘ΊπŸπŸ |
For a loss less network
= |π‘ΊπŸπŸ |
|π‘ΊπŸπŸ |𝟐 + |π‘ΊπŸπŸ |𝟐 = 𝟏
(𝟎. 𝟐)𝟐 + (𝟎. πŸ—)𝟐 ≠ 𝟏
The network is lossy and reciprocal.
Option (c)
14. In the circuit shown below, the network N is described by the following Y matrix:
𝑉
0.1𝑆 −0.01𝑆
π‘Œ=[
] The voltage gain 𝑉2 is
0.01𝑆
0.1𝑆
1
(a) 1/90
(b) -1/90
(c) -1/99
(d) -1/11
[GATE 2011: 2 Marks]
Soln.
25
I2
I1
+
+
100V
N
V1
-
π‘°πŸ = π’šπŸπŸ π‘½πŸ + π’šπŸπŸ π‘½πŸ
= 𝟎. 𝟎𝟏 π‘½πŸ + 𝟎. 𝟏 π‘½πŸ − − − − − − − (π’Š)
π‘½πŸ = −π‘°πŸ 𝑹𝑳 = −πŸπŸŽπŸŽπ‘°πŸ
π‘°πŸ =
−π‘½πŸ
𝟏𝟎𝟎
Substituting the value of I2 in equation (i)
−π‘½πŸ
𝟏𝟎𝟎
Or
= 𝟎. πŸŽπŸπ‘½πŸ + 𝟎. πŸπ‘½πŸ
π‘½πŸ
π‘½πŸ
=
−𝟏
𝟏𝟏
Option (d)
100
V2
-
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