Capacitive Voltage Divider

In this post I have explained how capacitive voltage divider circuits operate in electronic circuits, through formulas and solved examples.

By: Dhrubajyoti Biswas

What is a Voltage Divider Network

Talking about a voltage divider circuit, it is important to note that voltage in divider circuit gets equally distributed among all the existing components associated with the network, although the capacity may vary based upon the constitution of the components.

A voltage divider circuit can be built out of reactive components or even from fixed resistors.

However, when comparing to capacitive voltage dividers, the resistive dividers remain unaffected with the change of frequency in supply.

The purpose of this paper is to provide a detailed understanding of capacitive voltage dividers. But to gain more insight, it is vital to detail capacitive reactance and its effect on the capacitors at varied frequencies.

A capacitor is made of two conductive plates, placed parallel to each other which are additionally separated with an insulator. These two plates have one positive (+) and another negative (-) charge.

When a capacitor is charged fully via DC current, the dielectric [popularly referred to insulator] jams the current flow across the plates.

Another important characteristic of a capacitor in comparison to a resistor is: A capacitor stores energy on the conductive plates during charge, which the resistor does not, as it always tends to release out excess energy as heat.

But the energy stored by a capacitor is passed to the circuits that are connected with it during its discharge process.

This feature of a capacitor to store the charge is referred as reactance, and further referred as Capacitive Reactance [Xc] for which Ohm is the standard unit of measurement for reactance.

A discharged capacitor when connected to a DC power supply, the reactance remains low at the initial stage.

A substantial part of the current flows via the capacitor for a short span, which force the conductive plates get charged rapidly, and this eventually inhibits any further passage of current.

How Capacitor Blocks DC?

In a resistor, capacitor series network when the time period reaches a magnitude of 5RC, the conductive plates of the capacitor get fully charged, which signifies the charge received by the capacitor to be equal to the voltage supply, which stops any further current flow.

Furthermore, the reactance of the capacitor in this situation under the influence of the DC voltage reaches to max state [mega-ohms].

Capacitor in AC supply

In regard to using alternate current [AC] to charge a capacitor, wherein the AC current flow is always alternately polarized, the capacitor receiving the flow is subjected to a constant charging and discharging across its plates.

Now if we have constant current flow then we also need to determine the reactance value to restrict the flow.

Factors to determine value of capacitive resistance

If we take a look back on the capacitance we will find that the amount of charge on the conductive plates of a capacitor is proportional to the value of the capacitance and the voltage.

Now when a capacitor gets current flow from an AC input, the voltage supply goes through a constant change in its value, which invariably changes the value of the plates too proportionately.

Now let’s consider a situation where a capacitor contains higher value of capacitance.

In this situation the resistance R consume more time to charge the capacitor τ = RC. This implies that if the charging current is flowing for a longer span of time the reactance records a smaller value Xc, depending on the specified frequency.

Identically if the capacitance value is smaller in a capacitor, then to charge the capacitor it requires shorter RC time.

This shorter time causes the flow of current for a shorter span of time, which results in comparatively smaller reactance value, Xc.

Therefore, it is evident that with higher currents the value of the reactance remains small and vice versa.

And thus capacitive reactance is always inversely proportional to the capacitor’s capacitance value.

XC ∝ -1 C.

It is vital to note that capacitance is not the sole factor to analyze capacitive reactance.

With a low frequency of the AC voltage applied, the reactance gets more time develop based upon the allocated RC time constant. Further, it also blocks the current, indicating higher value of reactance.

Similarly, if the frequency applied is high, the reactance allows lesser time cycle for charging and discharging process to occur.

Moreover, it also receives higher current flow during the process, which leads to lower reactance.

So this proves that the impedance (AC reactance) of a capacitor and its magnitude is dependent on the frequency. Therefore, higher frequency results in lower reactance and vice versa, and thus it can be concluded that Capacitive Reactance Xc is inversely proportional to the frequency and capacitance.

The said theory of capacitive reactance can be summed up with the following equation:

Xc = 1/2πfC

Where:

· Xc = Capacitive Reactance in Ohms, (Ω)


· π (pi) = a numeric constant of 3.142 (or 22÷7)


· ƒ = Frequency in Hertz, (Hz)


· C = Capacitance in Farads, (F)

Capacitive Voltage Divider

This section will aim to provide a detailed explanation regarding how the frequency of supply affects two capacitors connected back to back or in series, better termed as capacitive voltage divider circuit.

Capacitive Voltage Divider Circuit

To illustrate a capacitive voltage divider functioning, let us refer to the circuit above. Here, C1 and C2 are in series and connected to an AC power supply of 10 volts. Being in series both the capacitors are receiving same charge, Q.

However, the voltage will remain different and it is also dependent on the value of capacitance V = Q/C.

Considering Figure 1.0, the calculation of voltage across the capacitor can be determined through different ways.

One option is to find out the total circuit impedance and circuit current, i.e. to trace the value of capacitive reactance on each capacitor and then calculate the voltage drop across them. For instance:

EXAMPLE 1

As per Figure 1.0, with C1 and C2 of 10uF and 20uF respectively, calculate rms voltage drops occurring across the capacitor in a situation of sinusoidal voltage of 10 volts rms @ 80Hz.

C1 10uF Capacitor
Xc1 = 1/2πfC = 1/2π x 80 x 10uF x 10-6 = 200 Ohm
C2 = 20uF capacitor
Xc1 = 1/2πfC = 1/2π x 8000 x 22uF x 10-6   = 90
Ohm

Total Capacitive Reactance

Xc(total) = Xc1 + Xc2 = 200Ω + 90Ω = 290Ω
Ct = (C1 x C2) / (C1 + C2) = 10uF x 22uF / 10uF + 22uF = 6.88uF
Xc = 1/2πfCt = 1 / 1/2π x 80 x 6.88uF = 290Ω

Current in the circuit

I = E / Xc = 10V / 290Ω

The voltage serially drops for both the capacitor. Here the capacitive voltage divider is calculated as:

Vc1 = I x Xc1 = 34.5mA x 200Ω = 6.9V
Vc2 = I x Xc2 = 34.5mA x 90Ω = 3.1V

If the values of the capacitors differ, the smaller value capacitor can then charge to a higher voltage in comparison to the large value one.

In Example 1, the voltage charge recorded is 6.9 & 3.1 for C1 and C2 respectively. Now since the calculation is based on Kirchoff’s theory of voltage, therefore the total voltage drops for individual capacitor equals to the supply voltage value.

NOTE:

The voltage drop ratio for the two capacitors that is connected to series capacitive voltage divider circuit always remains same even if there is a frequency in supply.

Therefore as per Example 1, 6.9 and 3.1 volts are the same, even if the supply frequency is maximized from 80 to 800Hz.

EXAMPLE 2

How to find the capacitor voltage drop using the same capacitors used in Example 1?

Xc1 = 1/2πfC = 1/2π x 8000 x 10uF = 2 Ohm

Xc1 = 1/2πfC = 1/2π x 8000 x 22uF = 0.9 Ohm

I = V/Xc(total) = 10/2.9 = 3.45 Amps

Therefore, Vc1 = I x Xc1 = 3.45A x 2Ω = 6.9V

And, Vc2 = I x Xc2 = 3.45A x 0.9 Ω = 3.1V

As the voltage ratio remains same for both the capacitors, with increasing supply frequency, its impact is seen in the form of a decrease of combined capacitive reactance, as well as for total circuit impedance.

A reduced impedance causes higher flow of current, for instance, the circuit current at 80Hz is around 34.5mA, whereas at 8kHz there may be a 10 times increase of current supply, that is around 3.45A.

So it can be concluded that the flow of current via capacitive voltage divider is proportional to the frequency, I ∝ f.

As discussed above, the capacitive dividers which involve series of capacitors connected, they all drop AC voltage.

To find out the correct voltage drop the capacitive dividers take the value of capacitive reactance of a capacitor.

Therefore, it does not work as dividers for DC voltage, since in DC the capacitors arrest and block current, which causes nil current flow.

The dividers can be used in cases where the supply is driven by frequency.

There is a wide range of electronic use of capacitive voltage divider, from finger scanning device to Colpitts Oscillators. It is also preferred extensively as cheap alternate for mains transformer where capacitive voltage divider are employed to drop high mains current.