Difference between revisions of "Voltage and Current Dividers"

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(Voltage division)
 
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In the circuit above,
In the circuit above,


<math>\frac{v_1}{v_s}=\frac{R_1}{R_1+R_2}</math>
<math>\frac{v_1}{v}=\frac{R_1}{R_1+R_2}</math>


or
or


<math>v_1=\frac{R_1}{R_1+R_2}v_s</math>
<math>v_1=\frac{R_1}{R_1+R_2}v</math>


We can generalize this equation for <math>N</math> number of resistances in series with the equation:
We can generalize this equation for <math>N</math> number of resistances in series with the equation:


<math>v_k=\frac{R_k}{R_1+R_2+\cdot\cdot\cdot+R_N}v_s</math>
<math>v_k=\frac{R_k}{R_1+R_2+\cdot\cdot\cdot+R_N}v</math>


where <math>v_s</math> is the voltage across the whole string of resistors.
where <math>v</math> is the voltage across the whole string of resistors.

==Current Division==
When we have a

Revision as of 11:38, 15 June 2006

Voltage Division

When we have a voltage source and resistors connected in series, we can express the voltage across a resistor as a ratio of voltages and resistances, without ever knowing the current.

File:Voltage division1.jpg

In the circuit above,

or

We can generalize this equation for number of resistances in series with the equation:

where is the voltage across the whole string of resistors.

Current Division

When we have a