The function is 1/ (R+jwRC) and the book I'm using said that the magnitude is 1/sqrt(1+(w/a)^2) were a=1/RC and the phase is -tan^-1(w/a). I have no idea how they got either answer and the book is no help. Please explain how to get it.
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hello Philip,
you should ask question properly. for example explain what the circuit is. sure it is some RC circuit but there can be several different connections - even for just two components.
suppose we have low pass filter for example
then Z1=R, Z2=1/(jwC) and in case of high pass filter Z1=1/(jwC) while Z2=R
output voltage is:
Vo=Vi*Z2/(Z1+Z2 (direct result of voltage divider equation).
by definition H=Vo/Vi
so in this case
H=Z2/(Z1+Z2)
then for low pass filter we get
H=[1/(jwC)] /[R+1/(jwC)]
H=[(1/jwC)] / [(jwRC+1)/jwC]
and finally after cancelling denominators we get
H=1/[1+jwRC)
if we define a=1/(RC)
we get
H=1/(1+jw/a) etc.
we can calculate magnitude different ways but result is the same.
simplest to do by hand is to do
h=magnitude of denominator
then
|H|= 1/h
where
h=sqrt(1^2+(w/a)^2)
so
|H|=1/sqrt(1^2+(w/a)^2)
and
tan(alpha)=imaginary part / real part
but since this is in denominator, angle is negative (you need to keep track of this when doing shortcuts like this; otherwise, do the expanded form where H=a+jb ann in this case you will get positive angle
tan(angle=b/a).
-tan(alpha)=(w/a) / (1)
which means
alpha=-arctan(w/a)
to get expanded form, you can multiply H by one (there are only two tricks in math: multiply by one, and add zero).
in our case we have transfer function in form
H=1/(u+jv)
to get normal form we multiply it by one where
1=(u-jv)/(u-jv)
note that u-jv is conjugate of denominator.
since we are multiplying by 1, H does not change but the representation will become a+jb.
you should ask question properly. for example explain what the circuit is. sure it is some RC circuit but there can be several different connections - even for just two components.
suppose we have low pass filter for example
then Z1=R, Z2=1/(jwC) and in case of high pass filter Z1=1/(jwC) while Z2=R
output voltage is:
Vo=Vi*Z2/(Z1+Z2 (direct result of voltage divider equation).
by definition H=Vo/Vi
so in this case
H=Z2/(Z1+Z2)
then for low pass filter we get
H=[1/(jwC)] /[R+1/(jwC)]
H=[(1/jwC)] / [(jwRC+1)/jwC]
and finally after cancelling denominators we get
H=1/[1+jwRC)
if we define a=1/(RC)
we get
H=1/(1+jw/a) etc.
we can calculate magnitude different ways but result is the same.
simplest to do by hand is to do
h=magnitude of denominator
then
|H|= 1/h
where
h=sqrt(1^2+(w/a)^2)
so
|H|=1/sqrt(1^2+(w/a)^2)
and
tan(alpha)=imaginary part / real part
but since this is in denominator, angle is negative (you need to keep track of this when doing shortcuts like this; otherwise, do the expanded form where H=a+jb ann in this case you will get positive angle
tan(angle=b/a).
-tan(alpha)=(w/a) / (1)
which means
alpha=-arctan(w/a)
to get expanded form, you can multiply H by one (there are only two tricks in math: multiply by one, and add zero).
in our case we have transfer function in form
H=1/(u+jv)
to get normal form we multiply it by one where
1=(u-jv)/(u-jv)
note that u-jv is conjugate of denominator.
since we are multiplying by 1, H does not change but the representation will become a+jb.
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