Objective. Students will apply Kirchhoff's Current Law (KCL) to a parallel resistor circuit, calculate branch currents and total current, and verify with DMM ammetery within ±5%.
This lesson, its worked examples and its practice questions has not yet been verified by an industry-certified professional or by a certification or approval body. It is a study draft and may contain errors. Do not use it as instructions for work on a job site or on live equipment. Always follow your instructor, your supervising professional, and current official references and regulations.
VoTechWorks program approval and accreditation are still in progress. Credentials are issued only by the certifying bodies named in each program, after their own exams.
In a parallel circuit, two or more components share the same two nodes—meaning each component is connected directly across the same voltage source. Every branch of a parallel circuit sees the same voltage, but each branch carries its own independent current. This is the defining characteristic that separates parallel circuits from series circuits.
Because each branch is a direct path across the supply, removing or opening one branch does not interrupt current flow through the remaining branches. This is why building wiring and most electronic power distribution use parallel connections.
Kirchhoff's Current Law states that the algebraic sum of all currents entering and leaving any node (junction) equals zero. A simpler way to say this: the total current flowing into a junction equals the total current flowing out.
For a parallel circuit with a DC supply:
I_total = I_1 + I_2 + I_3 + … + I_n
Where I_1, I_2, and I_3 are the individual branch currents. This follows directly from conservation of charge—charge cannot pile up at a node.
Because every branch shares the same supply voltage (V_supply), each branch current is found using Ohm's Law independently:
Total current drawn from the supply is then the sum of all branch currents.
Adding more parallel branches lowers total resistance because more paths are available for current. For two or more resistors in parallel, use the reciprocal formula:
1/R_total = 1/R_1 + 1/R_2 + 1/R_3
For exactly two resistors, the product-over-sum shortcut works:
R_total = (R_1 × R_2) / (R_1 + R_2)
Always verify: R_total must be less than the smallest individual resistor.
A digital multimeter (DMM) measures current by being placed in series with the branch being tested—the circuit must be physically broken, and the DMM is inserted into the break so all branch current flows through the meter. Key points:
1. Set the DMM to the correct DC current range before connecting (start high, work down).
2. Move the test lead to the correct current input jack on the DMM (often labeled A or mA).
3. Polarity matters: connect so conventional current enters the positive (COM) lead path and exits the negative lead, or the reading will be negative.
4. Never connect a DMM in ammeter mode directly across a voltage source—this is a short circuit and will blow the meter's internal fuse or damage the instrument.
Personal Protective Equipment (PPE): Safety glasses are required in the lab at all times when working with powered circuits or handling components that could be spring-loaded (e.g., breadboard springs under pressure).
Voltage Levels: The DC power supply used in this lab is low-voltage (typically 5–15 V DC). These levels are not normally a shock hazard to healthy adult skin, but good habits established now apply to higher-voltage work later in the program.
Power-Off Before Rewiring: Always turn off and, if the bench supply has a lockout provision, confirm it is de-energized before inserting or removing resistors from the breadboard. This prevents accidental short circuits that can damage components or trip supply protection.
Fuse Protection on DMM: If the ammeter leads are connected incorrectly (across a supply), the DMM fuse will likely blow. Report a blown fuse to the instructor immediately; do not guess at the replacement rating—use only the manufacturer-specified fuse type and rating.
Component Polarity: Standard resistors are not polarized; orientation does not matter. The DC power supply output terminals are labeled + and −; connect them correctly to maintain the intended current direction for meaningful KCL measurements.
During the lab, you will record five measurements: I_1, I_2, I_3, I_total (measured), and I_total (calculated from KCL). For each row, compute the percent deviation:
% deviation = |measured − calculated| / calculated × 100
A result within ±5% is acceptable given component tolerances (resistors are often ±5% or ±1%) and meter accuracy. If a reading is far outside this window, re-check meter lead placement and range setting before assuming a component is faulty.
For the concept-check portion, you will design your own two-branch circuit. Choose two resistors, predict R_total, I_total, I_1, and I_2 on paper first—write the KCL node equation—then build it on the breadboard and measure. Recording predictions before measuring is essential: it trains the habit of engineering estimation that employers expect of technicians.
KCL and parallel-circuit analysis appear on the ETA CET written examination and form the analytical foundation for understanding load distribution in telecom power plants, multi-drop wiring topologies, and network interface device (NID) circuits covered in BICSI Installer content. Solid mastery here pays off across all three credentials you will sit.
Answer each question, then check it. Nothing is recorded; this is your own practice.
A free tech program — complimentary, as our commitment to get America working. Help us build VoTechWorks. Tell us what works, what doesn’t, and what you want to learn.