How Do Inductors Function in Bandpass Filters Without Capacitors?

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SUMMARY

This discussion clarifies the function of inductors in bandpass filters without capacitors. It highlights that inductors can effectively cut off high frequencies while allowing low frequencies to pass, thus achieving bandpass characteristics. The derived transfer function T(jw) = \frac{-z}{(jwL + z)(jwL + R) } demonstrates how to select the impedance Z to meet resonant frequency requirements. The final formula for resonant frequency is f_{r} = \sqrt{f_{L} \cdot f_{H}}, with R_{z} calculated as R_{z} = \frac{100\pi^{2}L^{2}}{R}.

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  • Understanding of transfer functions in electrical circuits
  • Familiarity with inductors and their role in filtering
  • Knowledge of resonant frequency calculations
  • Basic proficiency in circuit analysis techniques
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  • Study the derivation of transfer functions in RLC circuits
  • Learn about the design and application of bandpass filters
  • Research resonant frequency and its significance in filter design
  • Explore practical applications of inductors in electronic circuits
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Electrical engineers, circuit designers, and students studying filter design and resonance in electronic systems will benefit from this discussion.

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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:
Untitled-1.jpg


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,

[tex]T(jw) = \frac{-z}{(jwL + z)(jwL + R)}[/tex]

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

If we select,

[tex]z = R_{z}[/tex]

We rearrange the transfer function,

[tex]\frac{-\frac{1}{R}}{(1 + \frac{jwL}{R_{z}})(1 + \frac{jwL}{R})}[/tex]

This becomes,

[tex]\frac{-\frac{1}{R}}{(1 + \frac{jw}{w_{L}})(1 + \frac{jw}{w_{H}})}[/tex]

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

[tex]f = 2\pi w[/tex]

Then our desired resonant frequency,

[tex]f_{r} = \sqrt{f_{L} \cdot f_{H}}[/tex]

Simply solve for, [tex]R_{z}[/tex].

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