Section 1 of 9Total resistance in series
When resistors are joined end to end, the current must pass through each one in turn, so the total opposition is greater than any single resistor. The total resistance of resistors in series is the sum of their resistances:
Rtotal = R1 + R2 + R3
The unit is ohms (Ω). Adding more resistors in series always increases the total resistance, and the total is larger than the biggest individual resistor.
Real circuits often contain resistors of the standard values 10, 22, 33, 47 and 100 Ω and so on, so you may need to combine two or three in series to obtain a value that is not available. For example, a 68 Ω requirement can be made from 47 Ω and 22 Ω, giving 69 Ω, close enough within the tolerance of the parts.
Section 2 of 9Why the resistances add
The current is the same everywhere in the loop, and the supply p.d. is divided among the resistors: V = V1 + V2 + V3.
Working out the total can also be done in reverse.
Section 3 of 9Method for series circuit problems
This method works for any number of resistors, and for components such as lamps that can be treated as resistors at a given operating point.
Be careful to use consistent units; if one resistor is in kΩ, convert it to Ω before adding. A 2.2 kΩ resistor is 2200 Ω. A frequent error is to add 2.2 and 330 without converting.
Section 4 of 9The potential divider
Two resistors in series form a potential divider, giving each a share of the supply p.d. proportional to its resistance. The larger resistor gets the larger p.d. If a fixed resistor is in series with an LDR, as the light level falls the LDR's resistance increases and so does its share of the p.d., which is used in switching circuits.
Section 5 of 9Practical use
Resistors in series are used to reduce the current, for example a 330 Ω resistor in series with an LED protects it from a large current.
In the dimmer example, as the slider increases the resistance, both the current and the brightness fall, and a larger share of the supply p.d. appears across the variable resistor instead of the lamp. If the total resistance is doubled while the p.d. is unchanged, the current halves. Resistance in series therefore acts as a control on current.
Section 6 of 9Checking with an experiment
Measure the resistance of two resistors separately, then connect them in series and measure again.
Section 7 of 9Worked examples
Resistors of 10 Ω, 22 Ω and 33 Ω are in series. Find the total resistance.
R = 10 + 22 + 33 = 65 Ω.
A 4.0 Ω resistor and a 8.0 Ω resistor are in series with a 6.0 V battery. Find the current and the p.d. across the 4.0 Ω resistor.
Rtotal = 12 Ω; I = 6.0/12 = 0.50 A.
V = IR = 0.50 × 4.0 = 2.0 V.
What the symbols mean: V = potential difference (V) · I = current (A) · R = resistance (Ω)A 12 V supply drives 0.20 A through two series resistors. One is 25 Ω. Find the other.
Rtotal = 12/0.20 = 60 Ω.
Other = 60 − 25 = 35 Ω.
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Total resistance | Single resistance with the same effect as the combination. |
| Series resistors | Resistors joined end to end in one loop. |
| Potential divider | Resistors in series that split voltage. |
| Tolerance | Allowed percentage difference from the marked value. |