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By: Carl H. Durney and Neil E. Cotter |
Filters |
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RLC filters |
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Frequency response |
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Example 3 |
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a. Choose values of L and C that will produce an ωo of 2π⋅104 and a Q of 2.
b. Calculate β, ωc1, and ωc2.
Ans: a) L = 3.2 mH, C = 80 nF
b) β = 31.4 k rad/s, ωC1 = 49.1 k rad/s, ωC2 = 80.5 k rad/s
Sol'n: a) This is a band reject filter with the following output:
The series L and C will act like a wire at the resonant frequency ωo and an open circuit for ω = 0 (where C acts like an open circuit) and ω → ∞ (where L acts like an open circuit):
The resonant frequency is found, as always, by solving for the frequency, ωo, where the impedance of the L plus the impedance of the C equals zero:
From the course text, we have an equation for the Q of this particular filter circuit:
(If necessary, we could also find Q by determining the cutoff frequencies where |H(jω)| = 1/√2. The difference of the cutoff frequencies is the bandwidth, β, and ωo/β = Q.)
Using the equations for ωo and Q, we do some algebra to find C:
Plugging in values given in the problem, we have
Rearranging the equation for Q and using this value of C gives the value for L:
or
Sol'n: b) From the course text or calculations of cutoff frequencies as described above, we have equations for cutoff frequencies that apply to simple RLC bandpass and bandreject filters:
Summing the equations gives a formula for bandwidth, β:
Now we compute ωC1, ωC2:
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Consistency check: