Calculate Impedance of AC Circuits with 1.20kΩ Resistor and 6.8μF Capacitor

  • Thread starter Thread starter airkapp
  • Start date Start date
  • Tags Tags
    Ac
AI Thread Summary
The discussion focuses on calculating the impedance of a series circuit consisting of a 1.20 kΩ resistor and a 6.8 μF capacitor connected to an AC source at frequencies of 60 Hz and 60,000 Hz. It clarifies that an inductance value is unnecessary since there is no inductor present in the circuit. The impedance can be calculated using the formula Z = R - j/(ωC), where ω is the angular frequency. The magnitude of the impedance is determined using |Z| = √(R² + (1/(ωC))²), and the phase angle can be found using φ = -arctan(1/(ωRC)). The discussion emphasizes the importance of treating impedances as complex quantities for accurate calculations.
airkapp
Messages
58
Reaction score
0
A 1.20 kΩ resistor and a 6.8 μF capacitor are connected in series to an AC source. Calculate the impedence of the circuit if the source frequency is a) 60 Hz, b) 60,000 Hz

I think I should this equation:

Vrms = Irms, Z : XL = 2ΠfL : XC = 1 / 2ΠfC

Z = √R2 + ( XL – XC )2 so: Irms = Vrms / Z

My main problem here is I don’t know how to do the equation without a given L. Do I need a given L (in Henry’s) to do the problem, and if I don’t, how else can I do it? Any help appreciated,
Thanks,
air
 
Physics news on Phys.org
airkapp said:
A 1.20 kΩ resistor and a 6.8 μF capacitor are connected in series to an AC source. Calculate the impedence of the circuit if the source frequency is a) 60 Hz, b) 60,000 Hz

I think I should this equation:

Vrms = Irms, Z : XL = 2ΠfL : XC = 1 / 2ΠfC

Z = √R2 + ( XL – XC )2 so: Irms = Vrms / Z

My main problem here is I don’t know how to do the equation without a given L. Do I need a given L (in Henry’s) to do the problem, and if I don’t, how else can I do it? Any help appreciated,
Thanks,
air

First: Read this again "A 1.20 kΩ resistor and a 6.8 μF capacitor are connected in series"

Second: what are the impedance equations?

Third: How do you deal with resistances in series circuits (impedance is analogous to resistance).

Finally: Reread this "Calculate the impedence of the circuit if the source frequency is a) 60 Hz, b) 60,000 Hz". RMS voltage or current are not required for this calculation.

Good luck.
 
airkapp said:
A 1.20 kΩ resistor and a 6.8 µF capacitor are connected in series to an AC source. Calculate the impedence of the circuit if the source frequency is a) 60 Hz, b) 60,000 Hz

I think I should this equation:

Vrms = Irms, Z : XL = 2ΠfL : XC = 1 / 2ΠfC

Z = vR2 + ( XL – XC )2 so: Irms = Vrms / Z

My main problem here is I don’t know how to do the equation without a given L. Do I need a given L (in Henry’s) to do the problem, and if I don’t, how else can I do it? Any help appreciated,
Thanks,
air

You only need an inductance if there's an inductor in the circuit. Here there is none.

It's best to deal with impedances as complex quantities since you can handle both magnitude and phase neatly in one step.

The impedance of the capacitor is \frac{-j}{\omega C}, a purely imaginary value.

The impedance of the resistor is just R, a real value.

The impedance of the series combination of the two is found just like in a d.c. circuit, by addition, giving a complex value :

Z = R - \frac{j}{\omega C}

The magnitude of the impedance is found like finding the magnitude of any complex number :

|Z| = \sqrt{R^2 + \frac{1}{{\omega}^2 C^2}}

The phase is found by getting the argument :

\phi = \arctan{\frac{\frac{-1}{\omega C}}{R}} = - \arctan{\frac{1}{\omega RC}}

Since \omega = 2\pi f where f is the given frequency, work out the magnitude and phase in each case, and you're done.

EDIT : Sorry for all the changes in the LaTex, I was having a tough time formatting it properly. It's fixed now.
 
Last edited:
Curious3141 said:
You only need an inductance if there's an inductor in the circuit. Here there is none.

It's best to deal with impedances as complex quantities since you can handle both magnitude and phase neatly in one step.

The impedance of the capacitor is \frac{-j}{\omega C}, a purely imaginary value.

The impedance of the resistor is just R, a real value.

The impedance of the series combination of the two is found just like in a d.c. circuit, by addition, giving a complex value :

Z = R - \frac{j}{\omega C}

The magnitude of the impedance is found like finding the magnitude of any complex number :

|Z| = \sqrt{R^2 + \frac{1}{{\omega}^2 C^2}}

The phase is found by getting the argument :

\phi = \arctan{\frac{\frac{-1}{\omega C}}{R}} = - \arctan{\frac{1}{\omega RC}}

Since \omega = 2\pi f where f is the given frequency, work out the magnitude and phase in each case, and you're done.

EDIT : Sorry for all the changes in the LaTex, I was having a tough time formatting it properly. It's fixed now.

thanks. That's what I thought about the inductance but I wasn't sure. I'm new to this. So the "i" is just imaginary. Everything else seems to just be math given the equations you gave me.

thanks again.
 
Last edited:
airkapp said:
thanks. That's what I thought about the inductance but I wasn't sure. I'm new to this. So the "i" is just imaginary. Everything else seems to just be math given the equations you gave me.

thanks again.

Instead of "i" (which can be confused with current), physicists use "j" to signify the square root of negative one.

Complex impedances are like phasors. A purely real impedance means the voltage and current are in phase. A purely imaginary impedance means the voltage and current are 90 degrees out of phase, which leads or lags depends on the sign of the impedance. A complex impedance means voltage and current are out of phase at some other angle.
 
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top