B What happens to the Low Pass Filter as frequency approaches 0 and infinity?

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As frequency approaches 0 in a low pass filter, the output approaches 1, indicating a DC open circuit for the capacitor. Conversely, as frequency approaches infinity, the output approaches 0, signifying that the capacitor acts as a short circuit. The discussion highlights the mathematical behavior of the filter function, specifically how terms in the equation influence the output at these limits. A misunderstanding about the behavior of the first term led to confusion regarding the output at DC. Ultimately, the analysis clarifies the expected outcomes for a low pass filter across varying frequencies.
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Low pass filter function

1/x(sqrt(R^2+1/(x^2)))

Just to show the limits as x approaches 0 and infinity, where x is frequency.
 
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Concise question ! Looks like homework, so PF culture requires some attempt at solution on your part. What do you propose ?
 
Self studier here, not enrolled in a course so HW is kind of a misnomer.

It should equal 1 at x = 0 ie DC, open circuit for capacitor and zero for frequency approaches infinity ie capacitor is short circuit.

It can't tho cos of the first term in x goes to 1/0 ie infinite at DC.
 
Self studier here
Kudos !

Simple recipe: for ##\ \ x\downarrow 0\ \ ## you want to be looking at something like ##\ \ A + x\ \ ## and for ##\ \ x\rightarrow\infty\ \ ## you want something like ##\ \ B + {1\over x}\ \ ##.

To wit for ##\ \ x\rightarrow\infty\ \ ##:$$ { 1\over x \sqrt{R^2+{1\over x^2}}}$$the last term in the denominator disappears besides R2 so you are left with ##1\over x R##.

For ##\ \ x\downarrow 0\ \ ## you bring the x inside the root: $${ 1\over \sqrt{x^2 R^2+1}}$$ and now the first term disappears besides the 1.
 
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thanks, I cast the problem of x approaching 0 as

(1/x)*1/(stuff)

and wrongly insisted that due to the first term (1/x) that the behaviour had to blow up to infinity.

I wanted the equation to fit my expectation even tho I knew the behaviour of the low pass in advance.
 
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