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Circuit Theory: Clarifying Source Power & Calculating No-Load Voltage with Thevenin's Theorem

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How do I determine the source-branch current and use Thevenin’s theorem to find the no-load voltage and branch current in this circuit?

For task 1, the source current is just the current through the source branch, and the correct value is 10 A; Thevenin’s theorem is not needed there [#16898183] For task 2, cut the branch with the 6 V source, find the equivalent resistance seen from terminals A–B as 6/5 Ω, and then solve the reduced circuit with the remaining 10 V source [#16906525][#16901995] After that, calculate the open-circuit voltage at the cut terminals from the reduced circuit, taking care with the voltage polarity because the directions do not simply add [#16904836][#16908741][#16908856] With the correct Thevenin voltage, the final result is I3 = 1.25 A [#16908926]
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  • #1 16898128
    Anonymous
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    #2 16898183
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  • #3 16898205
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  • #4 16901995
    kozi966
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    Thevenin's theorem is that you "cut" the branch in which you want to count something (in this case I3 current).
    From the point of view of this cut branch, you count the resistance for shorted voltage sources in the remaining circuit "after cutting" (in this case, one will remain ...).
    Then you calculate the voltage at the terminals from which you cut the branch (i.e. the voltage drop from the only source - on the resistance R4). So "we roll the circuit and develop."
    Having the voltage on the terminals, the replacement resistance, you substitute it as a new system with series connected: voltage source and resistance that you have just calculated.
    You now "add" a cut branch to their terminals and you have a simple circuit with a source voltage difference and two resistances.
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  • #6 16904434
    kozi966
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    You have calculated the replacement resistance,
    Now it's time to count the voltage in this system.
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  • #8 16904670
    kozi966
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    Erwin14 wrote:
    is it best to count and paste it here?

    With all due respect, but you must be kidding. Should I write the exam for you?

    I do not understand what you have a problem with when counting currents and voltages from one source.
    Since you only have E2, you add the resistances R4 and R5, then connect them in parallel with R1, and then in series with R2. Then pure oma law, and again we develop the circuit to find currents I1 and I2 (although here instead of currents, you immediately have the voltage on the corresponding elements).
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    #10 16904836
    kozi966
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    Erwin14 wrote:
    Is this the current I3 and the end of the task?

    No and no.
    So far, we have not yet come to the use of Thevenin's Theorem to the end.
    Now count the I2 current in your configuration. Multiply it by the resistance R4 and you have a voltage drop on the element that interests us (i.e. you are able to calculate the Uab voltage).
    Having the Uab voltage, having a substitute resistance, you have to make a substitute circuit to which you attach the previously cut branch, here:

    Circuit Theory: Clarifying Source Power & Calculating No-Load Voltage with Thevenin's Theorem

    This shows that it's bad You have marked current I3 at the moment.
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    #12 16906525
    kozi966
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    Unfortunately .... it's not good. The equivalent resistance seen from the viewpoint of terminals A and B is 6/5 ohms. As you stated in post # 5.
    In post # 9 is good. Because in post 9 you count the "second" system, with the 6V source cut out.
    You have calculated a replacement circuit with a 10V source (where the 3A source current comes out). You just need to develop it to know the voltage drop at the extreme right resistance:

    Circuit Theory: Clarifying Source Power & Calculating No-Load Voltage with Thevenin's Theorem

    If you know this voltage drop, this voltage drop is your substitute voltage in the Thevenin system.

    Only after that you create another layout to count, the one from post number # 10.

    PS
    In the circuit from post # 9 you have the error that you marked the current I3 as a current in the branch with a 10V source. Only that in the task, the current I3 (the correct one to count) is the current in the cut branch with a 6V source. From here you can get "mixed up".
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  • #14 16908856
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    Near!
    Just look at the direction of tensions ... they won't add up.
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  • #16 16908926
    kozi966
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    That's right
  • #17 16909148
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Topic summary

✨ The discussion revolves around solving circuit theory problems using Thevenin's Theorem, specifically focusing on calculating source power and no-load voltage. The user initially miscalculated the current in a branch with a voltage source, leading to confusion about the source current. Participants clarified that the source current is distinct from the current in the branch with the source. The conversation progressed to calculating equivalent resistance and no-load voltage, with various methods discussed, including Kirchhoff's equations. Ultimately, the correct current (I3) was determined to be 1.25 A, and the no-load voltage (Ez) was calculated as 2 V. The final solutions were compiled for future reference.
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FAQ

TL;DR: For this two-source exercise, the Thevenin resistance seen at A–B is 6/5 Ω; and “this voltage drop is your substitute voltage.” Apply Thevenin to get the target branch current. [Elektroda, kozi966, post #16906525]

Why it matters: This FAQ shows how to turn a messy mixed-source network into a one-source, two-resistor snap calculation—fast and exam-proof.

Quick-Facts

Quick Facts

What did “source power” mean in Task 1?

The forum clarified they wanted the source current, not power. Compute source power later as P = U × I if needed. In Task 1, the accepted result is 10 A and Thevenin is unnecessary. “And the source current is the source current.” [Elektroda, Anonymous, post #16898183]

How do I get the source current in Task 1 quickly?

Use Ohm’s law directly on the given source and its connected resistance. Thevenin reduction is not required here. The checked answer in the thread is 10 A for Task 1, matching a direct calculation approach. [Elektroda, Anonymous, post #16898183]

What is Thevenin’s theorem in plain words?

“You cut the branch” where you want the current, deactivate other sources appropriately, find the equivalent resistance and the open‑circuit voltage at the cut terminals, then reconnect the branch to this Thevenin pair to solve. [Elektroda, kozi966, post #16901995]

How do I compute the Thevenin resistance R_th at A–B here?

Cut the target branch, short the ideal voltage sources, and look into the network from A–B. For this circuit, R_th = 6/5 Ω. That numeric result was explicitly corrected and confirmed in the discussion. [Elektroda, kozi966, post #16906525]

What exactly is the no‑load (open‑circuit) voltage Ez/E0?

Ez is the terminal voltage Uab across A–B with the branch removed. In this problem, compute the drop at the rightmost resistor from the remaining active source; “this voltage drop is your substitute voltage.” [Elektroda, kozi966, post #16906525]

How do I calculate Uab (Ez) in this setup?

With the 6 V branch cut, keep the 10 V source active. Reduce the network, find current I2 through R4, then Ez = I2 × R4. The moderator’s guidance was to multiply I2 by R4 to obtain Uab. [Elektroda, kozi966, post #16904836]

Once I have Ez and R_th, how do I get I3?

Build the Thevenin equivalent (Ez in series with R_th), then reconnect the 6 V branch. Solve the resulting simple series network with correct polarity. The validated final result is I3 = 1.25 A. [Elektroda, kozi966, post #16908926]

Where did that 3 A come from in intermediate steps?

That 3 A is the source current when only the 10 V source drives the reduced network (R_Z2 ≈ 3.33 Ω). It’s an intermediate check, not I3. The helper notes “the 3A source current comes out” in that reduced case. [Elektroda, kozi966, post #16906525]

How do I avoid sign mistakes with voltages and currents?

Track source polarity and assumed current directions consistently. A reversed sign causes sums not to match. The helper flagged a misalignment with “look at the direction of tensions ... they won’t add up,” which required correction. [Elektroda, kozi966, post #16908856]

Can I solve Task 2 without Thevenin (e.g., with Kirchhoff)?

Yes. You can write node or loop equations for the full two‑source network and compute Uab and I3 directly. A participant did this, got results, then reworked to align with the requested Thevenin method. [Elektroda, Anonymous, post #16906351]

Give me a 3‑step How‑To for this exact circuit using Thevenin.

  1. Cut the 6 V branch; short other ideal voltage sources; compute R_th at A–B.
  2. With only the 10 V source active, find Uab = Ez at A–B.
  3. Build V_th = Ez in series with R_th, reconnect the 6 V branch, and solve for I3. [Elektroda, kozi966, post #16901995]

What is the target branch and current orientation for I3?

I3 is the current in the previously cut 6 V source branch, not in the 10 V source branch. Early confusion came from labeling I3 in the wrong branch; later posts corrected the assignment before confirming I3 = 1.25 A. [Elektroda, kozi966, post #16906525]

What edge case can flip my final answer?

If you reverse a source polarity relative to Ez, the Thevenin source and the branch source oppose or aid differently. That flips the sign of the net driving voltage and reverses I3’s direction, which the thread highlighted when fixing tension directions. [Elektroda, kozi966, post #16908856]

How can I sanity‑check numbers fast during an exam?

Estimate: with R_th ≈ 1.2 Ω and a small Ez, expect amperes only if Ez notably exceeds the branch source. Here, consistent orientation yielded I3 = 1.25 A, matching the discussed correction and confirmation. [Elektroda, kozi966, post #16908926]
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