Reduce a network by nodes rather than its drawing
Series elements share a current because no junction offers an alternative path between them.
Learning outcome: Redraw the same node connections in a different layout before calculating. Compare equal and unequal branches, retain the junction residual and one complete loop voltage account, and predict the open-branch limit without performing any physical switching.
Starting recap
Integrate current or resistance, preserve node topology and derive transient state with a signed energy account.
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Try
For branches 4 and 6 ohm, the parallel equivalent is 2.4 ohm and total is 4.4 ohm. At 12 V, common current is 30/11 A. Branch voltage is 72/11 V; currents are 18/11 and 12/11 A, which add to the common current.
Open the experimentPredict
What proves two branches are parallel?
Experiment
Redraw the same node connections in a different layout before calculating. Compare equal and unequal branches, retain the junction residual and one complete loop voltage account, and predict the open-branch limit without performing any physical switching.
Preserve topology while reducing a network
Worked teaching model · synthetic values · 12 V ideal source, 2 ohm common series resistor, then selected parallel branches returning to source. Nodes rather than drawing proximity define connectivity. No wire, meter or source resistance beyond stated components.
Reset keeps your prediction, captures and practice history.
Read the node connections before calculating
Two distinct branches connect J to B. Their drawing offsets do not change their shared endpoint nodes. Source positive terminal is S; conventional source-delivered current proceeds S to J. Component orientation and drawing lengths are schematic; source polarities are specified in the caption and node labels.
| First node | Second node | Element |
|---|---|---|
| S | J | 2 Ω |
| J | B | 4 Ω |
| J | B | 6 Ω |
| B | S | 12 V source |
Common schematic symbols and conventions
The symbol key is not a wiring recommendation. An open switch removes a conducting path; an ideal closed switch supplies a zero-drop connection. A current arrow is a chosen conventional-charge reference, not electron drift. A junction dot signifies connection; a crossing without a dot need not connect.
Potential around source-series-first-branch loop
Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.
Potential around source-series-first-branch loop: numerical coordinates
| ordered node index, not physical distance | potential (V) |
|---|---|
| 0 | 0 |
| 1 | 12 |
| 2 | 6.54545 |
| 3 | 0 |
| Quantity | Value | Unit |
|---|---|---|
| Parallel equivalent resistance | 2.4 | ohm |
| Total resistance | 4.4 | ohm |
| Common series current | 2.72727 | A |
| Parallel branch voltage | 6.54545 | V |
| First branch current | 1.63636 | A |
| Second branch current | 1.09091 | A |
| Junction residual | 0 | A |
| Series resistor power | 14.876 | W |
| First branch power | 10.7107 | W |
| Second branch power | 7.1405 | W |
| Total source power | 32.7273 | W |
The common current divides only at the actual junction, while both parallel branches share the same node-to-node voltage.
Series and parallel are connectivity relations, not horizontal or vertical placement in a drawing. Removing one branch increases equivalent resistance here. An ideal bypass across a resistor fixes its voltage to zero; an ideal zero-resistance path directly across an ideal source is a singular model, not a finite predicted current or a safe experiment.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
The common current divides only at the actual junction, while both parallel branches share the same node-to-node voltage.
Series and parallel are connectivity relations, not horizontal or vertical placement in a drawing. Removing one branch increases equivalent resistance here. An ideal bypass across a resistor fixes its voltage to zero; an ideal zero-resistance path directly across an ideal source is a singular model, not a finite predicted current or a safe experiment.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
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Public practice checks a specific claim. It does not establish independent mastery.
Which source, topology, initial condition or instrument assumption would invalidate this inference?
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