Difference between revisions of "Voltage and Current Dividers"
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==Voltage Division== |
==Voltage Division== |
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When we have a voltage |
When we have a voltage across a string of resistors connected in series, we can express the voltage across a single resistor as a ratio of voltages and resistances, without ever knowing the current. |
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[[Image:voltage_division1.jpg]] |
[[Image:voltage_division1.jpg]] |
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<math>v_1=\frac{R_1}{R_1+R_2}v</math> |
<math>v_1=\frac{R_1}{R_1+R_2}v</math> |
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We can generalize this equation for <math>N</math> number of |
We can generalize this equation for <math>N</math> number of resistors in series with the equation: |
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<math>v_k=\frac{R_k}{R_1+R_2+\cdot\cdot\cdot+R_N}v</math> |
<math>v_k=\frac{R_k}{R_1+R_2+\cdot\cdot\cdot+R_N}v</math> |
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==Current Division== |
==Current Division== |
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When we have a current flowing through resistors in parallel, we can express the current flowing through a single resistor as ratio of currents and resistances, without ever knowing the voltage. |
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When we have a |
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[[Image:current_division1.jpg]] |
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In the circuit above |
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<math>\frac{i_1}{i}=i\frac{R_2}{R_1+R_2}</math> |
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or |
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<math>i_1=\frac{R_2}{R_1+R_2}i</math> |
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where <math>i</math> is the current flowing through all the resistors. '''Note that the numerator on the right is R2, not R1.''' Remember that a larger resistance will carry a smaller current. |
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We can generalize the equation for <math>N</math> number of resistors in parallel with the equation: |
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<math>i_k=\frac{\frac{1}{R_k}}{\frac{1}{R_1}+\frac{1}{R_2}+\cdot\cdot\cdot+\frac{1}{R_N}}</math> |
Revision as of 11:53, 15 June 2006
Voltage Division
When we have a voltage across a string of resistors connected in series, we can express the voltage across a single resistor as a ratio of voltages and resistances, without ever knowing the current.
In the circuit above,
or
We can generalize this equation for number of resistors in series with the equation:
where is the voltage across the whole string of resistors.
Current Division
When we have a current flowing through resistors in parallel, we can express the current flowing through a single resistor as ratio of currents and resistances, without ever knowing the voltage.
In the circuit above
or
where is the current flowing through all the resistors. Note that the numerator on the right is R2, not R1. Remember that a larger resistance will carry a smaller current.
We can generalize the equation for number of resistors in parallel with the equation: