What is the emf of the ideal battery in this circuit?

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In summary, using KCL and the loop rule, the emf of the ideal battery in the given circuit is found to be 48.3 V.
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Homework Statement



What is the emf ##(\epsilon)## of the ideal battery in the following figure?

Homework Equations



##i_6 = 1.40 A##
##R_1 = R_2 = R_3 = 2.00 \Omega##
##R_4 = 16.0 \Omega##
##R_5 = 8.00 \Omega##
##R_6 = 4.00 \Omega##

The Attempt at a Solution



We can find the potential right away:

##V_6 = i_6R_6 = (1.40 A)(4.00 \Omega) = 5.6 V##

Note that ##i_5 = i_6## since ##R_5## and ##R_6## are in series, so we can find the other potential:

##V_5 = i_5R_5 = (1.40 A)(8.00 \Omega) = 11.2 V##

Now we note ##V_4 = V_5 + V_6 = 5.6 V + 11.2 V = 16.8 V## since the resistors are in parallel. Now ##i_4## can be found:

##i_4 = \frac{V_4}{R_4} = \frac{16.8 V}{16.0 \Omega} = 1.05 A##

By KCL once again, we have ##i_2 = i_4 + i_5 = 1.05 A + 1.40A = 2.45 A##. So that:

##V_2 = i_2R_2 = (2.45 A)(2.00 \Omega) = 4.90 V##

Now here is where I have a question. Would it be the case that ##R_2## and ##R_4## are in series? Then I would have ##R_3## in parallel and:

##V_3 = V_2 + V_4 = 4.90 V + 16.8 V = 21.7 V##

So that ##i_3 = \frac{V_3}{R_3} = \frac{21.7 V}{2.00 \Omega} = 10.85 A = 10.9 A##.

Appyling KCL again yields ##i_1 = i_2 + i_3 = 2.45 A + 10.85 A = 13.3 A##.

So we get ##V_1 = i_1 R_1 = (13.3 A)(2.00 \Omega) = 26.6 V##.

Appling the loop rule to the leftmost loop, we obtain:

##\epsilon - V_1 - V_3 = 0 \Rightarrow \epsilon = V_1 + V_3 = 26.6 V + 21.7 V = 48.3 V##.

Hence the emf is ##48.3 V##.
 

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  • #2
Zondrina said:

Homework Statement



What is the emf ##(\epsilon)## of the ideal battery in the following figure?

Homework Equations



##i_6 = 1.40 A##
##R_1 = R_2 = R_3 = 2.00 \Omega##
##R_4 = 16.0 \Omega##
##R_5 = 8.00 \Omega##
##R_6 = 4.00 \Omega##

The Attempt at a Solution



We can find the potential right away:

##V_6 = i_6R_6 = (1.40 A)(4.00 \Omega) = 5.6 V##

Note that ##i_5 = i_6## since ##R_5## and ##R_6## are in series, so we can find the other potential:

##V_5 = i_5R_5 = (1.40 A)(8.00 \Omega) = 11.2 V##

Now we note ##V_4 = V_5 + V_6 = 5.6 V + 11.2 V = 16.8 V## since the resistors are in parallel. Now ##i_4## can be found:

##i_4 = \frac{V_4}{R_4} = \frac{16.8 V}{16.0 \Omega} = 1.05 A##

By KCL once again, we have ##i_2 = i_4 + i_5 = 1.05 A + 1.40A = 2.45 A##. So that:

##V_2 = i_2R_2 = (2.45 A)(2.00 \Omega) = 4.90 V##

Now here is where I have a question. Would it be the case that ##R_2## and ##R_4## are in series?...
No. They're not in series, but applying the loop rule will give you ##\ V_3 = V_2 + V_4 \ .##


...Then I would have ##R_3## in parallel and:

##V_3 = V_2 + V_4 = 4.90 V + 16.8 V = 21.7 V##

So that ##i_3 = \frac{V_3}{R_3} = \frac{21.7 V}{2.00 \Omega} = 10.85 A = 10.9 A##.

Appyling KCL again yields ##i_1 = i_2 + i_3 = 2.45 A + 10.85 A = 13.3 A##.

So we get ##V_1 = i_1 R_1 = (13.3 A)(2.00 \Omega) = 26.6 V##.

Appling the loop rule to the leftmost loop, we obtain:

##\epsilon - V_1 - V_3 = 0 \Rightarrow \epsilon = V_1 + V_3 = 26.6 V + 21.7 V = 48.3 V##.

Hence the emf is ##48.3 V##.

Other than that it looks good.
 
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Related to What is the emf of the ideal battery in this circuit?

1. What is Quick Circuit Practice?

Quick Circuit Practice is a method used by scientists to quickly and efficiently test electronic circuits. It involves building a simplified version of a circuit using basic components and testing its functionality.

2. Why is Quick Circuit Practice important?

Quick Circuit Practice allows scientists to quickly assess the functionality of a circuit before investing time and resources into building a more complex version. It also helps in identifying any potential issues with the circuit design before moving on to the final build.

3. How is Quick Circuit Practice performed?

Quick Circuit Practice involves using basic electronic components such as resistors, capacitors, and transistors to build a simplified version of a circuit. The components are connected on a breadboard, and the circuit is tested using a power source and a multimeter to measure voltage and current.

4. What are the benefits of using Quick Circuit Practice?

Quick Circuit Practice allows scientists to save time and resources by identifying any flaws or issues with the circuit design before moving on to the final build. It also helps in improving the overall efficiency and functionality of the circuit.

5. Are there any limitations to Quick Circuit Practice?

Quick Circuit Practice is a simplified version of a circuit and may not accurately represent the functionality of the final build. It also does not account for factors such as heat dissipation and electromagnetic interference, which may affect the performance of the circuit in the final build.

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