At a junction, the total current equals the sum of the branch currents. Charge flow is conserved.
Example
At a junction, the total current equals the sum of the branch currents. Charge flow is conserved. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.
highlighted = computed this step
Current splits at the junction
The total current reaches the left bus, then splits between the two resistor branches. The branch currents depend on each branch resistance.
Itotal=IRa+IRb
At the same voltage, smaller branch resistance draws more current
Every branch gets 12 volts. A smaller branch resistance draws a larger current from that same voltage.
V12V12V12VR12ohm6ohm3ohmI1A2A4A
Compute each branch current
The upper branch carries 2 amperes and the lower branch carries 4 amperes.
branchRaRbV12V12VR6ohm3ohmI2A4A
The junction total is the branch-current sum
At the split, charge flow is conserved. Scan three possible branch pairs: the total current is always the two branch currents added.
IRa1A2A3AIRb2A4A6AItotal3A6A9A
Branch currents add to the total
At the junction, the 2 ampere upper-branch current plus the 4 ampere lower-branch current gives the 6 ampere total. The same values are drawn on the current arrows.
Itotal=2A+4A=6A
electricityA 12 V source across 6 ohm and 3 ohm branches gives branch currents of 2 A and 4 A, which add to 6 A at the junction.