790
Ω
0.01519
A
1.519
V
3.3418
V
7.1392
V
790
Ω
0.01519
A
1.519
V
3.3418
V
7.1392
V
Series resistor circuits are the simplest and most fundamental configuration in electronics — resistors connected end-to-end so that the same current flows through each component. The total resistance of a series circuit is simply the sum of all individual resistances: R_total = R1 + R2 + R3 + ... This direct addition makes series resistance calculation straightforward, and the circuit behavior highly predictable.
The governing principle of series circuits is Kirchhoff's Voltage Law (KVL): the sum of all voltage drops across resistors equals the applied supply voltage. Since the same current I = V / R_total flows through all resistors, each resistor's voltage drop is proportional to its resistance: V_n = I × R_n. A resistor twice as large as another carries the same current but has twice the voltage drop — this proportional voltage sharing is the principle behind voltage dividers.
Series resistors are used in numerous practical applications. Current limiting: a single series resistor limits the current through a load (LED, motor, solenoid) to a safe value. Voltage dropping: a series resistor creates a deliberate voltage drop to reduce supply voltage for a downstream component. Snubber circuits: series R-C networks across switch contacts absorb voltage spikes (dV/dt suppression) to prevent arcing. Pull-up and pull-down resistors: series or shunt resistors bias digital logic inputs to defined voltage levels when the driving output is disconnected (high impedance).
In analog circuit design, precision series resistors form voltage dividers for reference voltage generation, attenuators for signal level reduction, and Wheatstone bridges for sensor measurement. The tolerances of series resistors directly affect the accuracy of these circuits — ±1% resistors are commonly used for precision applications, while ±5% suffices for non-critical circuits.
Fault analysis in series circuits is simple: if one resistor opens (infinite resistance), the entire circuit current drops to zero and all supply voltage appears across the open component. If one resistor shorts (zero resistance), total resistance decreases, current increases, and other components face overvoltage and overcurrent stress — potentially causing cascading failures.
Temperature effects in series resistors are additive for small changes: each resistor's temperature coefficient contributes to the total resistance change. For temperature-stable voltage dividers, select resistors from the same batch and type (matched temperature coefficients), so both resistors in the divider change proportionally with temperature, keeping the ratio — and hence the output voltage — stable.
R_total = R1 + R2 + R3 + R4 (direct addition). Current I = V_supply / R_total. Voltage drops: V1 = I × R1, V2 = I × R2, V3 = I × R3. The sum V1 + V2 + V3 + V4 equals V_supply, confirming KVL. Set unused resistors to 0 to exclude them from the series chain.
Voltage drops are proportional to resistance values. The largest resistor carries the largest voltage drop. All voltage drops sum to the supply voltage. If V_drop_R1 > V_supply, check for input errors — individual drops cannot exceed total supply voltage in a purely series circuit.
Inputs
Results
A single 100 Ω series resistor on a 5 V supply limits current to 50 mA. With a 2 V LED forward drop, effective R should be (5-2)/0.02 = 150 Ω for 20 mA LED current.
Inputs
Results
A 100+220+470 Ω series chain on 12 V draws 15.2 mA. Drops are proportional: 100:220:470 ratio gives 1.52 V, 3.34 V, 7.14 V summing to 12 V.
Series: same current through all resistors, voltage divides proportionally. R_total = R1 + R2 (always greater than either alone). Parallel: same voltage across all resistors, current divides inversely. R_total = (R1×R2)/(R1+R2) (always less than either alone). Series increases resistance; parallel decreases resistance.
Sum the voltage drops from the reference (ground) to the node. V_node = V_supply - sum of drops across resistors between supply and the node. This is the principle of the voltage divider: V_out = V_in × R_lower / (R_upper + R_lower).
A larger series resistor reduces circuit current (I = V/R_total). LED brightness is approximately proportional to forward current. Too large a resistor starves the LED of current, reducing brightness. Too small a resistor allows excess current that can permanently damage the LED junction.
Contact resistance in connectors, switches, and solder joints adds directly to series circuit resistance. In low-resistance circuits (e.g., motor wiring, battery connections), even 10–50 mΩ of contact resistance causes significant voltage drop and heating at high currents. Clean contacts and proper torque on terminals minimize contact resistance.
High-voltage resistor dividers use series strings of standard resistors to distribute voltage below individual resistor breakdown ratings. A 100 kV measurement circuit might use 100 × 1 MΩ resistors in series, each seeing only 1 kV. Series connections also improve reliability through redundancy — partial failures degrade rather than catastrophically fail.
A bleeder resistor is connected in series from a high-voltage supply rail to ground. It draws a small continuous current to discharge capacitors safely when power is removed, provides a minimum load for voltage regulation stability, and slightly improves load regulation by providing a 'base load' for the regulator. Typical bleeder current is 10–25% of minimum rated load current.
Worst-case tolerance analysis: if R1 and R2 each have ±5% tolerance, the series combination can range from (R1+R2) × 0.95 to (R1+R2) × 1.05 — still ±5%. For ratio-sensitive applications (voltage dividers), use matched resistors with the same lot/date code — even ±5% resistors track each other closely when from the same batch.
Roboculator Team
The Roboculator Team explains calculations, planning tools, and practical formulas in clear language for real-life situations.
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