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Y/R by block reduction with G4 from input

Short answer

Y(s)/R(s) = G1G2G3/(1+G1G2H1+G2H1+G2G3H2) + G4.

Derive the overall transfer function Y(s)/R(s) for the system shown below using block reduction technique. [Figure: R(s) → node P → summing point S1 (+, −) → G1 → summing point S2 (+, −, −) → G2 → node B → G3 → node C → summing point S3 (+, +) → Y(s). G4 from node P (input R) to S3. H1 from node B fed back to both S1 (−) and S2 (−). H2 from node C fed back to S2 (−).]

Result: Y(s)R(s)=G1G2G31+G1G2H1+G2H1+G2G3H2+G4\dfrac{Y(s)}{R(s)} = \dfrac{G_1G_2G_3}{1+G_1G_2H_1+G_2H_1+G_2G_3H_2} + G_4

The diagram is reduced step by step using block diagram algebra rules (series, parallel, feedback, moving take-off points).

Step 1: Separate the parallel feed-forward path

G4G_4 takes the input RR directly to the output summing point S3S_3 (both inputs ++). So the system is two parallel paths:

Y(s)R(s)=C(s)R(s)+G4\frac{Y(s)}{R(s)} = \frac{C(s)}{R(s)} + G_4

where C(s)C(s) is the output of G3G_3 (node C). We now reduce the main path from RR to CC.

Step 2: Move the take-off point of H2H_2 from C to B

Node C is after G3G_3. Moving a take-off point before a block multiplies the branch by that block. So the H2H_2 feedback becomes G3H2G_3H_2 taken from node B.

Now two negative feedbacks go from B to S2S_2: H1H_1 and G3H2G_3H_2. They are in parallel:

Heq=H1+G3H2H_{eq} = H_1 + G_3H_2

Step 3: Reduce the inner loop around G2G_2

BE2=G21+G2(H1+G3H2)=G21+G2H1+G2G3H2\frac{B}{E_2} = \frac{G_2}{1+G_2(H_1+G_3H_2)} = \frac{G_2}{1+G_2H_1+G_2G_3H_2}

Step 4: Series with G1G_1, then the outer loop through H1H_1 to S1S_1

Forward path from S1S_1 to B: G1G21+G2H1+G2G3H2\frac{G_1G_2}{1+G_2H_1+G_2G_3H_2}, with negative feedback H1H_1:

BR=G1G21+G2H1+G2G3H21+G1G2H11+G2H1+G2G3H2=G1G21+G2H1+G2G3H2+G1G2H1\begin{aligned} \frac{B}{R} &= \frac{\frac{G_1G_2}{1+G_2H_1+G_2G_3H_2}}{1+\frac{G_1G_2H_1}{1+G_2H_1+G_2G_3H_2}} \\ &= \frac{G_1G_2}{1+G_2H_1+G_2G_3H_2+G_1G_2H_1} \end{aligned}

Step 5: Series with G3G_3 and add G4G_4

CR=G1G2G31+G1G2H1+G2H1+G2G3H2\frac{C}{R} = \frac{G_1G_2G_3}{1+G_1G_2H_1+G_2H_1+G_2G_3H_2}
        +------------ G4 -------------+
        |                             | +
 R ---->+--> [ G1G2G3 / Delta ] ----->(+)---> Y
                                        +
 Delta = 1 + G1G2H1 + G2H1 + G2G3H2
Y(s)R(s)=G1G2G31+G1G2H1+G2H1+G2G3H2+G4\frac{Y(s)}{R(s)} = \frac{G_1G_2G_3}{1+G_1G_2H_1+G_2H_1+G_2G_3H_2} + G_4

or, over a common denominator,

Y(s)R(s)=G1G2G3+G4(1+G1G2H1+G2H1+G2G3H2)1+G1G2H1+G2H1+G2G3H2\frac{Y(s)}{R(s)} = \frac{G_1G_2G_3 + G_4\left(1+G_1G_2H_1+G_2H_1+G_2G_3H_2\right)}{1+G_1G_2H_1+G_2H_1+G_2G_3H_2}

Check (Mason's rule): loops −G1G2H1-G_1G_2H_1, −G2H1-G_2H_1, −G2G3H2-G_2G_3H_2 all touch each other, so Δ=1+G1G2H1+G2H1+G2G3H2\Delta = 1+G_1G_2H_1+G_2H_1+G_2G_3H_2. Path G1G2G3G_1G_2G_3 touches all loops (Δ1=1\Delta_1=1); path G4G_4 touches none (Δ2=Δ\Delta_2=\Delta). This gives the same result.

✓ Answer checked by Claude Opus 5.5 (high effort)

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