The dB gain of cascaded systems is simply
The sum of the dB gains of each stage
In electronic systems, components are often connected in series, where the output of one stage becomes the input of the next. This is known as cascading. Examples include multi-stage amplifiers or signal processing chains. Each stage in a cascaded system contributes to the overall performance, including the gain or attenuation of the signal.
Gain is a measure of how much a signal is amplified or attenuated by a circuit or system. It can be expressed as a ratio or in decibels (dB).
Consider a system with two cascaded stages, Stage 1 and Stage 2. The output of Stage 1 is the input to Stage 2.
If the linear power gain of Stage 1 is \(G_1 = \frac{P_{out1}}{P_{in1}}\) and the linear power gain of Stage 2 is \(G_2 = \frac{P_{out2}}{P_{in2}}\), then the overall linear power gain \(G_{total}\) is the product of the individual gains:
\(G_{total} = \frac{P_{out2}}{P_{in1}}\)
Since the output of Stage 1 is the input to Stage 2 (\(P_{out1} = P_{in2}\)), we can write:
\(G_{total} = \frac{P_{out1}}{P_{in1}} \times \frac{P_{out2}}{P_{in2}} = G_1 \times G_2\)
For multiple cascaded stages (\(N\) stages), the total linear power gain is the product of the individual linear gains:
\(G_{total} = G_1 \times G_2 \times \dots \times G_N\)
Now, let's find the total gain in dB. Using the definition of dB gain:
\(G_{total, dB} = 10 \log_{10} (G_{total})\)
Substitute the expression for total linear gain:
\(G_{total, dB} = 10 \log_{10} (G_1 \times G_2 \times \dots \times G_N)\)
Using the logarithm property \(\log(A \times B) = \log(A) + \log(B)\):
\(G_{total, dB} = 10 \left( \log_{10}(G_1) + \log_{10}(G_2) + \dots + \log_{10}(G_N) \right)\)
\(G_{total, dB} = 10 \log_{10}(G_1) + 10 \log_{10}(G_2) + \dots + 10 \log_{10}(G_N)\)
Each term \(10 \log_{10}(G_i)\) is the dB gain of the individual stage \(G_{i, dB}\). Therefore:
\(G_{total, dB} = G_{1, dB} + G_{2, dB} + \dots + G_{N, dB}\)
This shows that the total dB gain of cascaded systems is the sum of the dB gains of each individual stage.
Similarly, for voltage or current gains in dB:
\(A_{V, total, dB} = 20 \log_{10} (A_{V, total}) = 20 \log_{10} (A_{V,1} \times A_{V,2} \times \dots \times A_{V,N})\)
\(A_{V, total, dB} = 20 \left( \log_{10}(A_{V,1}) + \log_{10}(A_{V,2}) + \dots + \log_{10}(A_{V,N}) \right)\)
\(A_{V, total, dB} = 20 \log_{10}(A_{V,1}) + 20 \log_{10}(A_{V,2}) + \dots + 20 \log_{10}(A_{V,N})\)
\(A_{V, total, dB} = A_{V,1, dB} + A_{V,2, dB} + \dots + A_{V,N, dB}\)
Thus, regardless of whether it's power, voltage, or current gain (using the appropriate \(10 \log_{10}\) or \(20 \log_{10}\) formulas), the total dB gain is the sum of the individual stage dB gains.
| Parameter | Linear Scale | dB Scale |
|---|---|---|
| Gain of Stage 1 | \(G_1\) | \(G_{1, dB}\) |
| Gain of Stage 2 | \(G_2\) | \(G_{2, dB}\) |
| ... | ... | ... |
| Gain of Stage N | \(G_N\) | \(G_{N, dB}\) |
| Total Gain (Cascaded) | \(G_{total} = G_1 \times G_2 \times \dots \times G_N\) | \(G_{total, dB} = G_{1, dB} + G_{2, dB} + \dots + G_{N, dB}\) |
Using the dB scale for gain in cascaded systems offers several advantages:
This fundamental property of dB gain being additive is crucial in analyzing complex multi-stage electronic systems.
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