Analysis of Resistors in Series and Parallel

Published: 26 February 2020 | Last Updated: 16 October 202515225
Several resistors are connected at a time to form a circuit without branches in the middle, which is called a resistor in a series circuit. And a circuit that connects two or more resistors between two points in a circuit with the same voltage at both ends of the resistor is called a resistor in a parallel circuit. The following mainly focus on the circuits, calculation methods, fault characteristics and fault treatment of resistors in series and parallel. And the final part introduces a concept-- ESR, which is related to series resistors and capacitors
Describes the rules governing the voltage, resistance and current for parallel circuits and series  circuits.

Resistors in Electric Circuits (1 of 16) Series vs. Parallel

Catalog

I Resistors in Series and Parallel Circuits

1. Resistors in Series Circuits

2. Resistors in Parallel Circuits

II Calculation of Series and Parallel Resistance

1. Calculation Example 1

2. Calculation Example 2

III Fault Characteristics and Treatment of Resistors in Series and Parallel

1. Features of Short Circuit and Open Circuit in Series Circuits

2. Fault Analysis of Series Resistors

3. Fault Detection of Resistors in Series

4. Failure Testing of Parallel Resistors

IV Equivalent Series Resistance(ESR)

I. Resistors in Series and Parallel Circuits

1. Resistors in Series Circuits

When resistors are connected end-to-end with no branches, they form a series circuit. The diagram below shows a series circuit with two resistors.

Resistor in Series Circuits

Resistors in Series Circuits

Key properties of series circuits:

(1) The current is the same through every component.

For n series resistors:

Resistance Formula 1-1

(2) The source voltage equals the sum of the voltage drops across each series resistor.

Resistance Formula 1-2

(3) The total (equivalent) resistance is the sum of all series resistances.

Replacing R1 and R2 by their equivalent R leaves current and node voltages unchanged.

Resistance Formula 1-4

(4) Voltage division and power in series:

Because the current is identical everywhere, each resistor’s voltage is proportional to its resistance, and the power dissipated by each is also proportional to its resistance.

Resistance Formula 1-4

Resistance Formula 1-5

Tip: Series resistors are commonly used as voltage dividers (e.g., to extend a voltmeter’s range). Always verify power ratings and add a safety margin.

2. Resistors in Parallel Circuits

Two or more resistors connected between the same two nodes (i.e., with the same voltage across them) form a parallel circuit.

Resistors in Parallel Circuits

Resistors in Parallel Circuits

Key properties of parallel circuits:

(1) Each branch has the same voltage.

Resistance Formula 2-1

(2) The total current equals the sum of branch currents.

Resistance Formula 2-2

(3) The inverse of the equivalent resistance equals the sum of inverses of branch resistances.

Resistance Formula 2-3

(4) Current division and power in parallel:

Because branch voltages are equal, branch current is inversely proportional to branch resistance. Branch power is also inversely proportional to resistance for a fixed branch voltage.

Resistance Formula 2-4

For two parallel resistors, the current division (shunt) formula is:

Resistance Formula 2-5

Note: Household lighting and appliance circuits are in parallel so that one device turning off or failing does not interrupt others.

II. Calculation of Series and Parallel Resistance

Complex resistor networks mix series and parallel groupings. Reduce them step-by-step using the same rules: combine series groups into sums and parallel groups using reciprocal sums. Remember: series elements share current; parallel elements share voltage.

1. Calculation Example 1

Find the total current drawn from a 12 V supply.

 Resistive Circuit Figure 3.

First, R2 and R3 are in series: R2 + R3 = 8 Ω + 4 Ω = 12 Ω. Replace them by 12 Ω (call this RA).

Resistance Formula 3-1

Now RA (12 Ω) is in parallel with R4 (12 Ω), giving R_comb = 6 Ω, then in series with R1 (6 Ω) for a total R_total = 12 Ω.

 Resistive Circuit Figure 4.

By Ohm’s law: I = V/R = 12 V / 12 Ω = 1 A.

 Resistive Circuit Figure 5.

Voltage drop on R1 is VR1=I·R1=1·6=6 V, leaving 6 V across the parallel pair. So branch currents are I1=6/12=0.5 A and I2=6/12=0.5 A; the supply current is 1 A (0.5 A + 0.5 A), consistent.

2. Calculation Example 2

Find the equivalent resistance REQ for the ladder network.

 Resistive Circuit Figure 6.

From the rightmost side, combine step by step (images preserved for each step):

 Resistive Circuit Figure 7.

Resistance Formula 4-1 (Formula 4-1)

Thus, RA + R7 = 4 + 8 = 12 Ω.

 Resistive Circuit Figure 8.

12 Ω in parallel with R6 gives RB=4 Ω, then RB + R5 = 4 + 4 = 8 Ω.

Resistance Formula 4-2 (Formula 4-2)

 Resistive Circuit Figure 9.

8 Ω in parallel with R4 yields RC=? (per diagram’s numeric values), then RC + R3 = 8 Ω (as shown in the original worked steps).

Resistance Formula 4-3 (Formula 4-3)

 Resistive Circuit Figure 10.

This 8 Ω is in parallel with R2, producing RD=4 Ω, then RD + R1 = 4 + 6 = 10 Ω, so REQ = 10 Ω.

Resistance Formula 4-4    
    Resistive Circuit Figure 11.

For networks that cannot be reduced by series/parallel (e.g., bridges, T-pads), use Kirchhoff’s laws, nodal/mesh analysis, or Δ–Y (delta–wye) transforms (see the Practical Add-Ons section).

III. Fault Characteristics and Treatment

1. Features of Short Circuit and Open Circuit in Series Circuits

(1) Short Circuit Features

If one series element becomes shorted (≈0 Ω), the total resistance drops and the series current increases (limited by the remaining series resistance and the source). This may overheat other components and the source.

Short Circuit in a Series Circuit

Short Circuit in a Series Circuit

  • Only the remaining resistors limit current; total current increases.

  • Voltage drops redistribute—less across the shorted element, more across the others (since current is larger).

  • Overcurrent can damage both components and the power supply.

(2) Open Circuit Features

An open circuit (infinite resistance) anywhere in a series path stops current everywhere. No current means ideal resistors have zero voltage drop; practically, the full source voltage appears across the open break (or across any device that became open).

Open Circuit in a Series Circuit

Open Circuit in a Series Circuit

2. Fault Analysis of Series Resistors

Illustrative summary for a two-resistor series string (R1–R2):

``````

ComponentFault TypeWhat You ObserveReasoning
R1Open CircuitSeries current is 0 A; no voltage drop across intact resistors; full source voltage appears across the open.No current → V=I·R=0 across intact resistors.
Short CircuitTotal resistance decreases; series current increases; R2 may overheat.Short reduces series resistance → higher current through R2.
Resistance IncreasedTotal resistance increases → current decreases. VR1=I·R1 may increase or decrease, but relative division shifts toward R1; VR2 decreases.Lower current, larger share of the (smaller) voltage drop goes to the larger resistor.
Resistance DecreasedTotal resistance decreases → current increases. VR1=I·R1 often decreases relative to before; VR2 increases.Higher current but much smaller R1 tends to reduce its share of the total drop.
Intermittent ContactCircuit behavior is unstable—sometimes normal, sometimes open/erratic.Contact resistance varies with vibration/temperature → intermittent series current.
R2Any of the aboveSymptoms mirror the R1 cases with components swapped.Apply the same logic swapping R1↔R2.

3. Fault Detection of Series Resistors

Use a multimeter (power off for resistance checks; appropriate DC/AC ranges for live voltage checks). Measuring voltage drops across series elements quickly reveals opens (0 A) and abnormal divisions due to drifted values.

Structure of a Multimeter

Structure of a Multimeter

(1) Open-Circuit Detection

In series, if any element is open, current is zero. With power on, you’ll typically see the full source voltage across the open location and ~0 V across intact resistors.

(2) Short-Circuit Detection

A short lowers total resistance and increases current. Compare measured total/branch currents and voltage drops against expected values. For safety, first measure resistance with power off if possible (to spot near-zero resistance where there should be some finite value).

4. Failure Testing of Parallel Resistors

(1) Open-Circuit Detection (Power Off)

Measure the total resistance of the parallel group. Normally, RTOTAL is less than the smallest branch resistor. If the measured value is higher than either branch value, one branch may be open. Branch currents (with power on) can confirm.

Detection of Open Circuit in Parallel Circuits

Detection of Open Circuit in Parallel Circuits

(2) Short-Circuit Detection (Power Off)

If measured total resistance is ~0 Ω, there is a shorted branch. With power on, that branch will carry disproportionally large current. Isolate branches to localize the fault.

IV. Equivalent Series Resistance (ESR)

ESR is the small, frequency-dependent resistance that appears in series with real capacitors (and inductors), arising from electrode/foil resistance, electrolyte, leads, and dielectric losses. Adding capacitors in series increases total ESR; adding them in parallel lowers ESR.

Because of ESR, a capacitor’s voltage can exhibit an instantaneous step equal to I × ESR at current transients, degrading filtering. Low-ESR capacitors improve ripple and transient response in power supplies, while some regulators actually require a minimum ESR range for loop stability.

Typical ESR magnitudes vary widely by technology, size, and frequency:

  • MLCC (ceramic): very low ESR (milliohms to a few tens of milliohms at high frequency).

  • Tantalum (MnO2): commonly ~0.1–2 Ω; polymer tantalum can reach tens of milliohms.

  • Aluminum electrolytic: legacy types may be >0.1–1+ Ω; low-ESR aluminum parts can also reach tens of milliohms at certain frequencies.

ESR also interacts with ESL (equivalent series inductance). Older wound capacitors had higher ESL; modern constructions reduce ESL, but at high frequencies ESL can dominate and produce resonances.

ESL and ESR Cancellation for Capacitors

ESL and ESR Cancellation for Capacitors

Ripple relation: for a ripple current I, ESR produces ripple voltage VESR = ESR × I. Reducing ESR or current ripple reduces output ripple.

Typical relationship between ESR and Frequency for Tantalum Capacitors

Typical ESR vs. Frequency (Tantalum)

Design notes (updated): check regulator datasheets for required ESR ranges; consider paralleling multiple capacitors (e.g., bulk electrolytic + MLCC) to lower net ESR/ESL; observe ripple current ratings and thermal derating.

V. Practical Add-Ons (2025 Update)

  • Δ–Y (Delta–Wye) Transform: For bridge-like networks, convert between delta and wye to enable series/parallel reduction.

  • Power Rating & Derating: Always ensure P=I²R=V²/R stays below the resistor’s rated power, with margin. Apply temperature derating per datasheet.

  • Temperature Coefficient (TCR): Precision resistors (e.g., metal-film, thin-film) have low TCR (e.g., ±5–50 ppm/°C) and are preferred for accurate dividers.

  • Tolerance & E-Series: Standard values follow E6/E12/E24… series. Match tolerance to application (e.g., 0.1% for precision sensing).

  • Noise: Carbon composition resistors are noisier than metal-film/thin-film. For low-noise designs, prefer metal-film and keep resistor values moderate.

  • Paralleling Resistors: In high-power designs, use equal values in parallel to share current; place them thermally symmetrically.

  • Measurement Safety: Measure resistance with power removed and capacitors discharged. For live measurements, start with the highest meter range.

Recommended Articles

What is a Variable Resistor?

Understanding of Carbon Film Resistors

Beginners Guide to Precision Resistors

What are the Differences Between Pull-Up and Pull-Down Resistors? 

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Frequently Asked Questions

1.How do you find the resistance of a resistor in a series circuit?

If two resistors or impedances in series are unequal and of different values, then the total or equivalent resistance, RT is equal to the mathematical sum of the two resistances. That is equal to R1 + R2.

2.How do you find the current through a resistor in parallel and series?

The current through the circuit is the same for each resistor in a series circuit and is equal to the applied voltage divided by the equivalent resistance: I=VRS=9V90Ω=0.1A. Note that the sum of the potential drops across each resistor is equal to the voltage supplied by the battery.

3.How do you find the total resistance in a series parallel circuit?

The sum of the currents through each path is equal to the total current that flows from the source. You can find total resistance in a Parallel circuit with the following formula: 1/Rt = 1/R1 + 1/R2 + 1/R3 +... If one of the parallel paths is broken, the current will continue to flow in all the other paths.

4.What determines if the resistors are in series or parallel?

There are two quantities that determine if resistors are connected in series or parallel - Current and Voltage. ... If the voltage across the resistors connevted is the same then they are said to be connected in parallel.

5.How do you calculate resistors in series?

To calculate the total overall resistance of a number of resistors connected in this way you add up the individual resistances. This is done using the following formula: Rtotal = R1 + R2 +R3 and so on. Example: To calculate the total resistance for these three resistors in series.
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