1 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 2 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 3 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 4 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: In the above circuit at node 1, π1 − ππ ππ ππ − 0 = 2πΌ1 + + 8 2 4 π1 −ππ But πΌ1 = therefore 8 π1 − ππ 3ππ 0= + 8 4 0 = π1 − ππ + 6ππ => π1 = −5ππ −5ππ − ππ πβπ’π , πΌ1 = = −0.75ππ 8 πΌ1 πππ π¦11 = = 0.15π π1 At node 2, (ππ − 0) + 2πΌ1 + πΌ2 = 0 4 −πΌ2 = 0.25ππ − 1.5ππ = −1.25ππ πΌ2 π»ππππ π¦21 = = −0.25π π1 Chapter 16: Two-Port Networks 5 Irwin, Engineering Circuit Analysis, 11e ISV Similarly we get y21 and y22 using the figure. We get π¦12 = −0.05π πππ π¦22 = 0.25π Chapter 16: Two-Port Networks 6 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 7 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 8 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 9 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 10 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 11 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 12 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: This reciprocal network is shown as below: Replacing the blocks with equivalent elements Chapter 16: Two-Port Networks 13 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 14 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 15 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 16 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 17 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 18 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 19 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 20 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 21 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 22 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: This is not a reciprocal network. We may use the equivalent circuit in the figure. Writhing the equations π1 = 40πΌ1 + π20πΌ2 π2 = π30πΌ1 + 50πΌ2 Substituting V1 and V2 as π1 = 100∠0, π2 = −10πΌ1 Thus the equation becomes 100 = 40πΌ1 + π20πΌ2 −10πΌ1 = π30πΌ1 + 50πΌ2 => πΌ1 = π2πΌ2 Thus solving these two equations 100 = π80πΌ2 + π20πΌ2 => πΌ2 = −π Thus πΌ1 = 2∠0π΄, πΌ2 = 1∠ − 90π΄ Chapter 16: Two-Port Networks 23 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 24 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 25 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Determinant of the matrix is β= 37 π΄ 10 β 37 π§11 = = = 5, π§12 = = = 18.5 πΆ 2 πΆ 2 1 1 π· 4 π§21 = = = 0.5, π§22 = = = 2 πΆ 2 πΆ 2 5 18.5 [π] = [ ] 0.5 2 Chapter 16: Two-Port Networks 26 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 27 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 28 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 29 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 30 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 31 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 32 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 33 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 34 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 35 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 36 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: To find h11 and h21, we short circuit the output port and connect a current source I1 and to the input port as shown. V1 = I1 (2 + 3||6 ) = 4I1 π Hence β11 = 1 = 4β¦ πΌ1 Also by current division 6 2 −πΌ2 = πΌ1 = πΌ1 6+3 3 πΌ2 2 π»ππππ β21 = = − πΌ1 3 To obtain h12 and h22, we open circuit the input port and connect voltage source V2 to the output port as given in figure. By voltage division 6 2 π1 = π2 = π2 6+3 3 π1 π»ππππ β12 = π2 Also π2 = (3 + 6)πΌ2 = 9πΌ2 Chapter 16: Two-Port Networks 37 Irwin, Engineering Circuit Analysis, 11e ISV β22 = πΌ2 1 = π π2 9 Chapter 16: Two-Port Networks 38 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 39 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 40 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 41 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 42 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 43 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 44 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 45 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 46 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 47 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 48 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 49 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 50 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 51 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 52 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 53 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 54 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 55 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 56 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 57 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 58 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 59 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Let us refer upper network as Na and lower as Nb. The two networks are connected in parallel. π¦12π = −π4 = π¦21π , π¦11π = 2 + π4, π¦22π = 3 + π4 Or 2 + π4 −π4 [π¦π ] = [ ]π −π4 3 + π4 And π¦12π = −4 = π¦21π , π¦11π = 4 − π2, π¦22π = 4 − π6 4 − π2 −4 [π¦π ] = [ ]π −4 4 − π6 6 + π2 −4 − π4 [π¦] = [π¦π ] + [π¦π ] = [ ]π −4 − π4 7 − π2 Chapter 16: Two-Port Networks 60 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 61 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 62 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 63 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 64 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 65 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: π§22 0.4 = 2.5, βπ = π¦11 π¦22 − π¦21 π¦12 = 0.5 × 0.4 − 0.2 × 0.2 = 0.16 βπ 0.16 π¦12 0.2 π§12 = − = = 1.25 = π21 βπ 0.16 π¦11 0.5 π22 = = = 3.125 βπ 0.16 π§11 = Chapter 16: Two-Port Networks 66 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 67 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 68 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 69 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 70 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: The circuit is the cascade connection of the two T networks. A T network has the following network parameters. π 1 π 1 (π 2 + π 3 ) 1 π 3 π΄ = 1 + , π΅ = π 3 + ,πΆ = ,π· = 1 + π 2 π 2 π 2 π 2 Applying this to cascaded networks, we get π΄π = 1 + 4 = 5, π΅π = 8 + 4 × 9 = 44, πΆπ = 1, π·π = 1 + 8 = 9 And 5 44 [ππ ] = [ ] 1 9 Similarly 1 6 [ππ ] = [ ]π 0.5 4 Thus for total network 27 206 π] = [ππ ][ππ ] = [ ] 5.5 42 Chapter 16: Two-Port Networks 71 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: To determine A and C, we leave the output port open as shown in figure so that I2 = 0 and place a voltage source V1 at the input port. We have π1 = (10 + 20)πΌ1 = 30πΌ1 π2 = 20πΌ1 − 3πΌ1 = 17πΌ1 π1 πΌ1 πβπ’π π΄ = = 1.765 πππ πΆ = = 0.0588π π2 π2 To obtain B and D we short circuit the output port so that V2 = 0 as shown in circuit. We place a voltage source V1 at the input port. At node a in the circuit, π1 − ππ ππ − + πΌ2 = 0 10 20 π −π But ππ = 3πΌ1 and πΌ1 = 1 π . 10 Combining these gives Chapter 16: Two-Port Networks 72 Irwin, Engineering Circuit Analysis, 11e ISV ππ = 3πΌ1 πππ π1 = 13πΌ1 Substituting Va = 3I1 and replacing first term with I1 in the previous equation 3πΌ1 17πΌ1 πΌ1 − + πΌ2 = 0 => = −πΌ2 20 20 πΌ1 20 Therefore, π· = − = = 1.176 πΌ2 17 π1 13πΌ1 π΅=− =− = 15.29β¦ 17 πΌ2 − πΌ1 20 Chapter 16: Two-Port Networks 73 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 74 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 75 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 76 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 77 Irwin, Engineering Circuit Analysis, 11e ISV Chapter 16: Two-Port Networks 78 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 79 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 80 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: Chapter 16: Two-Port Networks 81 Irwin, Engineering Circuit Analysis, 11e ISV SOLUTION: The circuit which is obtained by following the definitions of h parameters is following. Chapter 16: Two-Port Networks