The above figure shows a circuit made with two identical resistors, R = 1 k Ω and two identical capacitors C = 1 μ F . The input voltage is V i n = A cos ω t V . Find the value of ω (in rad/sec) at which the amplitude of the output voltage V o u t is maximum, for a given fixed input amplitude A .
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Great analysis. Thanks for sharing it.
Let Z 1 = j ω C 1 ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ( R + j ω C 1 ) , the C-C-R π circuit on the right. Then the impedance of the whole RC circuit is Z = R + Z 1 . And we have:
V i n V o u t = Z Z 1 × R + j ω C 1 R = R + Z 1 Z 1 × 1 + j ω C R j ω C R = R + 2 j ω C R − ω 2 C 2 R 1 + j ω C R 2 j ω C R − ω 2 C 2 R 1 + j ω C R × 1 + j ω C R j ω C R = 1 − ω 2 C 2 R 2 + j ω C R ( 1 + 2 R ) 1 + j ω C R × 1 + j ω C R j ω C R = 1 + 2 R + j ( ω C R − ω C R 1 ) 1 See note: Z 1 = 2 j ω C R − ω 2 C 2 R 1 + j ω C R
For the same ∣ V i n ∣ , ∣ V o u t ∣ is maximum , when ∣ ∣ ∣ ∣ 1 + 2 R + j ( ω C R − ω C R 1 ) ∣ ∣ ∣ ∣ is minimum or
ω C R − ω C R 1 ω 2 C 2 R 2 ω C R ⟹ ω = 0 = 1 = 1 = C R 1 = 1 0 − 6 × 1 0 3 1 = 1 0 0 0 rad/s
Note:
Z 1 = j ω C 1 ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ( R + j ω C 1 ) = j ω C 1 + R + j ω C 1 j ω C 1 ( R + j ω C 1 ) = 2 j ω C R − ω 2 C 2 R 1 + j ω C R
Excellent analysis. Thanks for sharing this explanation.
Sweep over the angular frequency and plot the gain at each value of ω .
Z C = − ω C j Z 1 = R + Z C Z 2 = Z 1 + Z C Z 1 Z C V 1 = V i n R + Z 2 Z 2 V o u t = V 1 R + Z C R Gain = ∣ ∣ ∣ V i n V o u t ∣ ∣ ∣
The gain has a maximum value of 3 1 at ω = 1 0 0 0 rad/s . This is not really a low-pass filter since it rejects DC. I will therefore call it a band-pass filter.
A great solution. Thanks for sharing it.
You're welcome, and thanks for the problem. May I use the graphic for a followup problem?
Absolutely.
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Not an expert at Latex, neither am one in circuit analysis. My approach involves the use of the concept of transfer functions.