Prove Thevenin's Theorem: Annoying But Necessary

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The discussion centers on the Thevenin equivalent circuit, which simplifies analysis by allowing a load to see two circuits as identical. The origin and proof of Thevenin's theorem are questioned, contrasting it with Kirchhoff's laws, which have clear foundational proofs. The conversation explains that the Thevenin equivalent can be represented as a voltage source in series with a resistance, while the Norton equivalent is a current source in parallel with a resistance. Both representations yield the same voltage-current characteristics when specific relationships between the resistances and sources are maintained. Understanding these relationships clarifies the equivalence of the two models in circuit analysis.
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Using thevenin equivalent is very good way to simply the circuit, because we know that the load can't "tell" the different between 2 circuits. But the thevenin's origin is really troublesome. I really don't know how to prove the thevenin's theorem or what's state of it. Kirchhoff Law has proof itself (electron into and out of a node must be equal). Node and Mesh current method are base on that proof too. But thevenin's theorem is different. It's really really annoy me! Please tell me how to prove it or which origin lead to thevenin's theorem...
 
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this is really an electrical engineering question. but the answer is pretty much what you said in your first sentence. put a voltage source of voltage V_T in series with resistance R_T in a black box and pull the two terminals out. now what is the "volt-amp" characteristic of that two terminal devices (the V-I characteristics fully describe the device, at least as far as the outside world is concerned)? if you define current coming out of the + terminal as positive (that is usually opposite of how we define it for loads), you will see that the V-I characteristic is

V = V_T - R_T I

now do the same thing for a "norton source", an ideal current source I_N in parallel with a resistance R_N and pull the two terminals out. now what is the V-I characteristic?

I = I_N - \frac{V}{R_N}

or

V = R_N(I_N - I) = R_N I_N - R_N I

now you can easily see that the V-I characteristic of the two "different" 2 terminal devices are exactly the same if R_N = R_T and V_T = R_N I_N = R_T I_N.
 
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