Electronics - RC Circuits - Discussion
Discussion Forum : RC Circuits - General Questions (Q.No. 3)
3.
What is the voltage drop across R1 in the given circuit?
Discussion:
20 comments Page 1 of 2.
Alex said:
1 decade ago
No. Just simply, no.
You guys are all doing this wrong and the answers are wrong.
You can't simply combine the parallel R2||Xc2 in the traditional method. You have to remember that capacitive reactance is at an angle of -90°.
When you combine that parallel branch, you have to convert back and forth between polar and rectangular forms as appropriate (addition in rectangular, multiplication/division in polar).
So let me walk you through this:
Req=R2||X2.
Req=333||-j250.
Req=1/((1/333)+(1/250<-90°)) <--in polar for division.
Req=1/(0.003+j 0.004) <--in rectangular for addition.
Req=1/(0.005<53°) <--Convert to a vector/rectangular.
Req=200<-53° <-- That is the equivalent resistance.
Now, convert that back to rectangular and add R1 and Xc1:
200<-53° = 120-j159.73.
Zt = (120-j159.73)+(180-j240).
Zt = 300-j400 <-- (rounded to -j400).
Zt = 500<-53° <-- (polar representation).
Now:
It = Vt/Zt=10V/500<-53°) = 0.02 A < 53°.
VR1 = It*R1 = 0.02 A*180Ω = 3.6 V.
You guys are all doing this wrong and the answers are wrong.
You can't simply combine the parallel R2||Xc2 in the traditional method. You have to remember that capacitive reactance is at an angle of -90°.
When you combine that parallel branch, you have to convert back and forth between polar and rectangular forms as appropriate (addition in rectangular, multiplication/division in polar).
So let me walk you through this:
Req=R2||X2.
Req=333||-j250.
Req=1/((1/333)+(1/250<-90°)) <--in polar for division.
Req=1/(0.003+j 0.004) <--in rectangular for addition.
Req=1/(0.005<53°) <--Convert to a vector/rectangular.
Req=200<-53° <-- That is the equivalent resistance.
Now, convert that back to rectangular and add R1 and Xc1:
200<-53° = 120-j159.73.
Zt = (120-j159.73)+(180-j240).
Zt = 300-j400 <-- (rounded to -j400).
Zt = 500<-53° <-- (polar representation).
Now:
It = Vt/Zt=10V/500<-53°) = 0.02 A < 53°.
VR1 = It*R1 = 0.02 A*180Ω = 3.6 V.
Divyanshu Shekhar said:
9 years ago
I think here XL1 = 240 ohm not XC 1=240 ohm.
When XL 1 = 240 ohm, then calculate:
z1 = 180 + j240
z2 = 333 * -j250/(333-j250)
= 120.03 -j159.88
= 120-j160 (approx.)
z = z1 + z2
= 300 + j80
z = sqrt[(300)2 + (80)2]
=310.48 ohm = 310.5 ohm(approx.).
i = v/z = 10/310.5 = 0.0322 A.
Voltage drop across r1 = 180 * 0.0322.
= 5.79 volts.
= 5.8 volt(approx).
Also, phase angle, tan(θ) = 80/300 = 0.26666 = 0.267(approx).
So, θ = Arctan(0.267).
= 14.95 degree.
When XL 1 = 240 ohm, then calculate:
z1 = 180 + j240
z2 = 333 * -j250/(333-j250)
= 120.03 -j159.88
= 120-j160 (approx.)
z = z1 + z2
= 300 + j80
z = sqrt[(300)2 + (80)2]
=310.48 ohm = 310.5 ohm(approx.).
i = v/z = 10/310.5 = 0.0322 A.
Voltage drop across r1 = 180 * 0.0322.
= 5.79 volts.
= 5.8 volt(approx).
Also, phase angle, tan(θ) = 80/300 = 0.26666 = 0.267(approx).
So, θ = Arctan(0.267).
= 14.95 degree.
Samar said:
7 years ago
Here;
1. Get the inverse (1/333 - 1/250i)^-1 to get the impedance since it is in admittance form, then it will be equal to 120.03 + 159.88i.
2. Then next step is to add that to (180 - 240i).
3. And, (120.03 + 159.88i) + (180 - 240i) = 300.09 - 80.12i.
4. Then convert that to Polar form which is equal to 310.55 <-14.95.
5. Now the total impedance is 310.55, and by voltage divider formula Vr1 = (10/310.55)(180) = 5.8 volts.
1. Get the inverse (1/333 - 1/250i)^-1 to get the impedance since it is in admittance form, then it will be equal to 120.03 + 159.88i.
2. Then next step is to add that to (180 - 240i).
3. And, (120.03 + 159.88i) + (180 - 240i) = 300.09 - 80.12i.
4. Then convert that to Polar form which is equal to 310.55 <-14.95.
5. Now the total impedance is 310.55, and by voltage divider formula Vr1 = (10/310.55)(180) = 5.8 volts.
(3)
Rose said:
9 years ago
I want an answer to my question.
Suppose we have a circuit where the ratio of the complex amplitude of the particular integral to the amplitude of the driving sinusoid is
VpVi = jωRC1 + jωRC.
Given that R = 0.82kΩ and C = 10.0nF we will compute the magnitude and phase of this ratio for various frequencies.
For frequency f = 170Hz what is the magnitude of VpVi?
Suppose we have a circuit where the ratio of the complex amplitude of the particular integral to the amplitude of the driving sinusoid is
VpVi = jωRC1 + jωRC.
Given that R = 0.82kΩ and C = 10.0nF we will compute the magnitude and phase of this ratio for various frequencies.
For frequency f = 170Hz what is the magnitude of VpVi?
Shahid said:
1 decade ago
Hey friends let me explain.
For rc SERIES circuit Z=Sqrt of R^2+xC^2
R2 is parallel to 250 so it will be 142.79
It is in series with 180 so total res Rt will be 322.79
Now use formula=z=sqrt(322.79^2+240^2)=402.23
Now we have I=V/Z=0.0248
Now vtg drop across r1=0.024*(180/180+240)=5.78v
For rc SERIES circuit Z=Sqrt of R^2+xC^2
R2 is parallel to 250 so it will be 142.79
It is in series with 180 so total res Rt will be 322.79
Now use formula=z=sqrt(322.79^2+240^2)=402.23
Now we have I=V/Z=0.0248
Now vtg drop across r1=0.024*(180/180+240)=5.78v
Farhan said:
1 decade ago
@Shahid.
You are doing totally wrong, Now you see your step where you find the voltage drop across R1 you use current divider formula that's wrong applied. You use voltage divider instead of current divider.
Vdrop_R10= (R10) *VSupply /Total Resistance of the circuit.
You are doing totally wrong, Now you see your step where you find the voltage drop across R1 you use current divider formula that's wrong applied. You use voltage divider instead of current divider.
Vdrop_R10= (R10) *VSupply /Total Resistance of the circuit.
Ajayvignesh said:
1 decade ago
Raja you are wrong. R2 is not parallel to summation of all three. its parallel to only XC2. Hence parallel reistance is 142.8Ohm. Hence drop across 142.8 (equivalanet resistance of 333Ohm and XC2 250Ohm) is
Abhiee said:
10 years ago
Let me tell in more simpler way.
R1 and XC1 are series to source. So z1 = sqrt (R1^2+XC1^2).
R2 and XC2 are parallel to source. So z2 = 1/sqrt ((1/R2)^2+(1/XC2)^2).
Then z = z1+z2. Voltage drop = R1/z*vs.
R1 and XC1 are series to source. So z1 = sqrt (R1^2+XC1^2).
R2 and XC2 are parallel to source. So z2 = 1/sqrt ((1/R2)^2+(1/XC2)^2).
Then z = z1+z2. Voltage drop = R1/z*vs.
(1)
Scott said:
1 decade ago
I = V/Req.
Zt = R1+XC1+R2 parallel with XC2.
Zt = 500 ohm @ -53.1 degrees.
It = 10v/500 ohm @ -53.1 degrees = 20 mA @ 53.1 degrees.
Vr1 = 180 ohms @ 0 degrees * 20 mA @ 53.1 degrees = 3.6 V @ 53.1 degrees.
Zt = R1+XC1+R2 parallel with XC2.
Zt = 500 ohm @ -53.1 degrees.
It = 10v/500 ohm @ -53.1 degrees = 20 mA @ 53.1 degrees.
Vr1 = 180 ohms @ 0 degrees * 20 mA @ 53.1 degrees = 3.6 V @ 53.1 degrees.
Sangamesh said:
1 decade ago
Since the parallel combination of xc2 and R2 = 142.79.
Therefore z = square root(180^2+240^2+142.79^2) = 332.25.
Hence Vr1 = 10*180/332.25 = 5.8v.
Therefore z = square root(180^2+240^2+142.79^2) = 332.25.
Hence Vr1 = 10*180/332.25 = 5.8v.
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