How Do Inductors Function in Bandpass Filters Without Capacitors?

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Inductors can function in bandpass filters without capacitors by utilizing their ability to cut off high frequencies, while the circuit's design allows for the desired frequency response. The transfer function derived for this circuit is T(jw) = -z/((jwL + z)(jwL + R)), where selecting an appropriate impedance Z is crucial for achieving the resonant frequency. By rearranging the transfer function, the relationship between the resonant frequency and the circuit components can be established, leading to the formula for resonant frequency f_r = √(f_L · f_H). The calculation of R_z, which is essential for the filter's performance, is given by R_z = 100π²L²/R. This discussion highlights the viability of designing bandpass filters using only inductors.
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Can I get some help with this? I don't even know where to begin.
 
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dillonmhudson said:
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Can I get some help with this? I don't even know where to begin.

Bandpass filters usually employ both inductors and capictors.

The inductor cuts off the high frequencies, while the capacitor cuts off the low frequencies, ideal for a bandpass filter.
 
jegues said:
Bandpass filters usually employ both inductors and capictors.

The inductor cuts off the high frequencies, while the capacitor cuts off the low frequencies, ideal for a bandpass filter.

Whoops, I just noticed that the the answer is given in the figure. I can see they did not use a capacitor!

I managed to derive the transfer function for this circuit and found the following,

T(jw) = \frac{-z}{(jwL + z)(jwL + R)}

Now we simply need to select our Z such that the requirement for resonant frequency is obatined.

If we select,

z = R_{z}

We rearrange the transfer function,

\frac{-\frac{1}{R}}{(1 + \frac{jwL}{R_{z}})(1 + \frac{jwL}{R})}

This becomes,

\frac{-\frac{1}{R}}{(1 + \frac{jw}{w_{L}})(1 + \frac{jw}{w_{H}})}

Now we know what wL and wH are we can solve for fL and fH since,

f = 2\pi w

Then our desired resonant frequency,

f_{r} = \sqrt{f_{L} \cdot f_{H}}

Simply solve for, R_{z}.

You should find that, R_{z} = \frac{100\pi^{2}L^{2}}{R}
 
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