At the loaded output node, the incoming source current splits exactly into the bottom-branch current and the load-branch current, and KCL must close for every row. The three rows give source currents of 2, 12/5, and 8/3 A as the sum of their two branch currents exactly for the ideal node model; real nodes add resistor tolerance, source impedance, loading, contact resistance, heating, supply limits, temperature drift, and current measurement uncertainty.

The output node current split closes by exact KCL for every load row. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

The output node is a current-sum checkpoint

At the loaded output node, source current splits into bottom current and load current. The helper checks that split before the diagram is rendered.

Is=Ib+ILI_s=I_b+I_L
Loaded-divider KCLThe current arrows meet at the output node.12 V3 ohm6 ohm6 ohm2 A1 A1 A+-6 V+-6 V+-6 Voutput

Every row closes the node current sum

The source current column equals the bottom-branch current plus the load-branch current in each row.

IbILIs1 A1 A2 A45 A85 A125 A23 A2 A83 A\begin{array}{c|c|c}I_b&I_L&I_s\\1\ \text{A}&1\ \text{A}&2\ \text{A}\\\tfrac{4}{5}\ \text{A}&\tfrac{8}{5}\ \text{A}&\tfrac{12}{5}\ \text{A}\\\tfrac{2}{3}\ \text{A}&2\ \text{A}&\tfrac{8}{3}\ \text{A}\\\end{array}
Loaded-divider KCLThe rendered row has one ampere in each branch.12 V3 ohm6 ohm6 ohm2 A1 A1 A+-6 V+-6 V+-6 Voutput

The first row splits two amperes into one plus one

For the rendered row, the source current is 2 amperes, and the two outgoing branch currents are each 1 ampere.

1 A+1 A=2 A1\ \text{A}+1\ \text{A}=2\ \text{A}
Loaded-divider KCLThe displayed current arrows close the node sum.12 V3 ohm6 ohm6 ohm2 A1 A1 A+-6 V+-6 V+-6 Voutput