In electronics, the voltage divider rule, or simply the voltage divider, resistor divider or potential divider, is a design technique used to create a voltage (Vout) which is proportional to another voltage (Vin).
Two resistors are connected as shown in the following diagram:
The output voltage Vout is related to Vin as follows:
As a simple example, if R1 = R2 then
Any ratio between 0 and 1 is possible.
Note that this rule only works if the divider is unloaded, i.e. the load resistance is infinite and all of the current flowing through R1 goes into R2. If current flows into a load resistance (through Vout), that resistance must be considered in parallel with R2 (see resistor) to determine the voltage at Vout.
A voltage divider is usually thought of as two resistors, but capacitors, inductors, or any combined impedance can be used. For general impedances Z1 and Z2, the voltage becomes
For instance, a divider can be made with a resistor and capacitor:
The resistor's impedance is simply its resistance:
The capacitor's impedance is a large resistance at low frequencies and a low resistance at high frequencies. The exact formula is:
where j is the imaginary unit, and ω is frequency in radians per second. This divider will then have the voltage ratio:
The ratio then depends on frequency, in this case decreasing as frequency increases. This circuit is, in fact, a basic (first-order) lowpass filter, or, in the world of audio, a treble-cut filter. The ratio contains an imaginary number, and actually contains both the amplitude and phase shift information of the filter. To extract just the amplitude ratio, calculate the magnitude of the ratio, or just use the reactance of the capacitor instead of the impedance.
Dělič napětí | Spændingsdeler | Spannungsteiler | Divisor de tensión | Diviseur de tension | Įtampos daliklis | Dzielnik napięcia | Divisor de tensão
This article is licensed under the GNU Free Documentation License.
It uses material from the
"Voltage divider rule".
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