Robin Barton

 
 

Resistor Circuits

Resistors are commonly combined in one of the following configurations: Series, Parallel or Bridge. These circuits are discussed below.

Series Resistors

If the resistors are connected in series, the total resistance is equal to the sum of the individual resistances i.e.:

RTotal = R1 + R2 + ... + Rn

Example:  Three resistors are connected in series.
They have values of: 1kΩ, 2kΩ and 3kΩ.

RTotal = 1kΩ + 2kΩ + 3kΩ
= 6kΩ

Series resistors are often used as voltage dividers to provide a reference voltage of a fixed percentage of the supply voltage. Below is an interactive example.

⚠ The application of these circuits requires careful consideration as the load can affect the effective resistance of the part of the divider that it is connected across - see parallel resistors.

Resistance:   Ω Ω    RTotal:
 
Circuit: Ⓐ— R1 ———┬——— R2 —Ⓑ Current:
  
Voltage:   VR1   VR2
 V VV



Parallel Resistors

If resistors are connected in parallel, the total resistance is equal to the inverse of the sum of the inverse of the individual resistances i.e.:

⅟RTotal = ⅟R1 + ⅟R2 + ... + ⅟Rn

Example:  Three resistors are connected in parallel.
They have values of: 1kΩ, 2kΩ and 3kΩ.

⅟ RTotal = ⅟1kΩ + ⅟2kΩ + ⅟3kΩ
= 545.455Ω
 
☀Handy Hint:The result will always be less than the lowest resistor value.

Parallel resistors are often used to obtain non-preffered resistance values i.e. where a value is required that cannot be bought off the shelf or as current dividers (shunts). Parallel resistance calculations also come into play when you introduce a load across part of a voltage divider. Below is an interactive example.

  Ω 
  R1  
Circuit:  Ⓐ— —Ⓑ 
  R2  
  Ω 

Is equivalent to:
 
Circuit:  Ⓐ— Ω—Ⓑ 



Resistor Bridge

Resistor Bridges are generally used for measurement circuits for example Wheatstone Bridge circuits. Normally one of the resistors would be replaced with a device such as a thermistor or light dependant resistor. They combine series and parallel resistances.

V: V
 
  Ω Ω 
  R1 R2  
V:   VXY V V:
Ⓐ——Ⓑ
 
R3 R4  
  Ω Ω 
 
V: V

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