Difficulty: Easy
Correct Answer: an equivalent current source in parallel with an equivalent impedance
Explanation:
Introduction / Context:
Norton's theorem is a cornerstone of circuit simplification in electrical engineering. It allows you to replace any linear, bilateral two-terminal network (containing independent/dependent sources and resistances/impedances) with an equivalent model that is easier to analyze—especially for varying loads and parallel interconnections.
Given Data / Assumptions:
Concept / Approach:
Norton's theorem states that a two-port seen from its output terminals is equivalent to a current source IN in parallel with an impedance RN (also written ZN). IN is the short-circuit current at the terminals, and RN equals the Thevenin resistance RTH (found by deactivating independent sources, or by test-source methods when dependent sources are present).
Step-by-Step Solution:
Verification / Alternative check:
Convert between Thevenin and Norton to verify: VTH = IN * RN and RTH = RN. Analyzed with any load RL, the Norton and Thevenin forms yield identical terminal currents and voltages.
Why Other Options Are Wrong:
'Voltage source in series with impedance' is Thevenin, not Norton. 'Current source in series with impedance' is not a standard canonical form. 'Voltage source in parallel with impedance' also does not match Norton's canonical form.
Common Pitfalls:
Confusing IN with load current (IN is the short-circuit current), and forgetting that RN equals RTH. Also, failing to treat dependent sources correctly when computing RN.
Final Answer:
an equivalent current source in parallel with an equivalent impedance
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