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George Mason University Volgenau School of Engineering Department of Electrical and Computer Engineering
Lab 5 Report
ECE 285-
Alexander Ing
Contents
1 Thevenin’s Theorem 1 1.1 Theory and Calculations............................................ 1 1.2 Simulation.................................................... 2
2 Norton’s Theorem 4 2.1 Theory and Calculations............................................ 4 2.2 Simulation.................................................... 5
3 Conclusion 5
Figure 1.1: Circuit for Lab 5
1 Thevenin’s Theorem
1.1 Theory and Calculations
A. Find the theoretical Thevenin’s voltage VTh by finding the open-circuit voltage between terminals a and b for the circuit in Figure 1.1. Solution In order to find the theoretical Thevenin’s voltage VTh, we can use the redrawn circuit in Figure 1.2 and
Figure 1.2: Redrawn circuit from Figure 1.1 to find VTh
find the voltage at the terminals of R 3. The equivalent resistance in this circuit is expressed by summing the resistors R 1 , R 3 , and R 4 :
Req = 1 kΩ + 2.2 kΩ + 3 kΩ = 6.2 kΩ
Then, the current through the loop can be found by applying Ohm’s Law:
I =
V
R
⇒ I =
10 V
Req
≈ 1 .61 mA
Lastly, we can apply Ohm’s Law again to find the voltage across this resistor.
VTh = IR 3 = (1.61 mA)(2.2 kΩ) ≈ 3 .55 V
B. Then find the theoretical Thevenin’s resistance RTh by removing the Load Resistor. Also replace the source V 1 with its internal resistance (ideally, a short). Solution To find the theoretical Thevenin’s resistance RTh, we can use the redrawn circuit in Figure 1.3 and solve for the equivalent resistance between terminals a and b.
Rab ≡ RTh = R 2 + (R 3 ‖ (R 1 + R 4 )) + R 5 = 3 kΩ + (2.2 kΩ ‖ (1 kΩ + 3 kΩ)) + 10 kΩ ≈ 14 .4 kΩ
4 3
0
Title
Size
Date:
A
Title
Size
Date:
A
Title
Size
Date:
A
R_Th
14.4k
204 .0uA
V_Th
204 .0uA
LOAD
3k
204 .0uA
3.550V
a
612.1mV
b
0V
Figure 1.5: Thevenin equivalent circuit simulation
4 3 2
R
3k
203 .7uA
R
2.2k
1.482mA
R
1k
1.685mA
V
1.685mA
LOAD
3k
203.7uA
R
10k
203.7uA
R
3k
1.685mA
10.00V 8.315V
b 0V 5.056V 7.093V
a 7.704V
Figure 1.6: Original circuit simulation
2 Norton’s Theorem
2.1 Theory and Calculations
A. Calculate the Norton’s resistance RN for the circuit in Figure 1.1. How is it related to Thevenin’s resistance RTh? Solution Norton’s equivalent resistance RN is calculated using the same process as RTh, thus it is the exact same. See part B from section 1.1 for the work.
RN ≡ RTh ≈ 14 .4 kΩ
B. Also calculate the Norton’s current IN for the circuit in Figure 1.1. Solution The Norton current IN can be calculated from our previously calculated values of VTh and RTh.
IN =
VTh RTh
3 .55 V
14 .4 kΩ
≈ 0 .247 mA
C. Draw the Norton’s equivalent circuit and calculate the voltage across the load resistor. Solution The Norton equivalent circuit is shown in Figure 2.1. As for the voltage across the load resistor, we must
4 3 2
Title
Size Documen
</p> <h4>A</h4> <p>Title</p> <p>Size Documen <Doc></p> <p><Title></p> <h4>A</h4> <p>Title</p> <p>Size Documen <Doc></p> <p><Title></p> <h4>A</h4> <h4>I_N</h4> <p>246.5u</p> <h4>LOAD</h4> <p>3k</p> <h4>R_N</h4> <p>14.4k</p> <p>Figure 2.1: Norton equivalent circuit</p> <p>first calculate the equivalent resistance in the circuit.</p> <p>Req = RN ‖ Rload =</p> <p>14 .4 kΩ × 3 kΩ 14 .4 kΩ + 3 kΩ</p> <p>≈ 2 .48 kΩ</p> <p>Now, we can use Ohm’s Law to calculate the voltage across the parallel combination of everything.</p> <p>V = IR ⇒ Vab = IN Req ≈ 611 mV</p> </div></div></div></div><footer id="footer" class="sc-gsnTZi hxUvtc"><div width="100%" display="grid" class="sc-gsnTZi sc-breuTD hQDdiS hAbyOH"><div class="sc-gsnTZi sc-ksZaOG hINUYJ ijDdyb"><p color="muted" class="sc-dkzDqf jtFJUi">University</p><div width="100%" display="grid" class="sc-gsnTZi sc-breuTD jxbiSy ddZtgY"><div class="sc-gsnTZi sc-ksZaOG hINUYJ dPsdkt"><a href="/en/university/us/" color="negative" class="sc-dkzDqf 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_3\"\u003e\u003c/span\u003er\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ey\u003cspan class=\"_ _0\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ed\u003cspan class=\"_ _4\"\u003e\u003c/span\u003eC\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ec\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eu\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003et\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eo\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _3\"\u003e\u003c/span\u003es............................................\u003cspan class=\"_ _5\"\u003e \u003c/span\u003e1\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e\u003c/div\u003e\u003cdiv class=\"t m0 x8 h6 yb ff5 fs4 fc0 sc0 ls0 ws7\"\u003e1\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e.\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e2\u003cspan class=\"_\"\u003e \u003c/span\u003eS\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003em\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eu\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003et\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eo\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _4\"\u003e\u003c/span\u003e....................................................\u003cspan class=\"_ _5\"\u003e \u003c/span\u003e2\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e\u003c/div\u003e\u003cdiv class=\"t m0 x7 h8 yc ff7 fs4 fc0 sc0 ls1 ws6\"\u003e2\u003cspan class=\"_ _1\"\u003e \u003c/span\u003eNorton’s\u003cspan class=\"_\"\u003e \u003c/span\u003eTheorem\u003cspan class=\"_ _6\"\u003e \u003c/span\u003e4\u003c/div\u003e\u003cdiv class=\"t m0 x8 h6 yd ff5 fs4 fc0 sc0 ls0 ws7\"\u003e2\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e.\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e1\u003cspan class=\"_\"\u003e \u003c/span\u003eT\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eh\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ee\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eo\u003cspan class=\"_ _3\"\u003e\u003c/span\u003er\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ey\u003cspan class=\"_ _4\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ed\u003cspan class=\"_ _0\"\u003e\u003c/span\u003eC\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ec\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eu\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003et\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eo\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _3\"\u003e\u003c/span\u003es............................................\u003cspan class=\"_ _5\"\u003e \u003c/span\u003e4\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e\u003c/div\u003e\u003cdiv class=\"t m0 x8 h6 ye ff5 fs4 fc0 sc0 ls0 ws7\"\u003e2\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e.\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e2\u003cspan class=\"_\"\u003e \u003c/span\u003eS\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003em\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eu\u003cspan class=\"_ _3\"\u003e\u003c/span\u003el\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ea\u003cspan class=\"_ _3\"\u003e\u003c/span\u003et\u003cspan class=\"_ _3\"\u003e\u003c/span\u003ei\u003cspan class=\"_ _3\"\u003e\u003c/span\u003eo\u003cspan class=\"_ _3\"\u003e\u003c/span\u003en\u003cspan class=\"_ _4\"\u003e\u003c/span\u003e....................................................\u003cspan class=\"_ _5\"\u003e \u003c/span\u003e5\u003cspan class=\"_ _3\"\u003e\u003c/span\u003e\u003c/div\u003e\u003cdiv class=\"t m0 x7 h8 yf ff7 fs4 fc0 sc0 ls1 ws8\"\u003e3\u003cspan class=\"_\"\u003e \u003c/span\u003eConclusion\u003cspan class=\"_ _7\"\u003e \u003c/span\u003e5\u003c/div\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:106.380654px;bottom:1152.946732px;width:118.767000px;height:7.911000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:136.659346px;bottom:1124.797516px;width:131.641000px;height:9.848000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:136.659346px;bottom:1104.499608px;width:70.676000px;height:7.911000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:106.380654px;bottom:1060.090588px;width:108.251000px;height:7.911000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:136.659346px;bottom:1031.943399px;width:131.641000px;height:9.848000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" style=\"border-width:1.000000px;border-style:solid;border-color:rgb(255,0,0);position:absolute;left:136.659346px;bottom:1011.645490px;width:70.676000px;height:7.911000px;background-color:rgba(255,255,255,0.000001);\"\u003e\u003c/div\u003e\u003c/span\u003e\u003cspan class=\"l\"\u003e\u003cdiv class=\"d m1\" 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w0 h0","width":"1240","height":"1604.705882"},{"className":"pf w0 h0","width":"1240","height":"1604.705882"},{"className":"pf w0 h0","width":"1240","height":"1604.705882"},{"className":"pf w0 h0","width":"1240","height":"1604.705882"},{"className":"pf w0 h0","width":"1240","height":"1604.705882"},{"className":"pf w0 h0","width":"1240","height":"1604.705882"}],"sizes":[{"width":"1240","height":"1604.705882","numberOfPages":6}]},"documentText":"\u003cp\u003eGeorge Mason University Volgenau School of Engineering Department of Electrical and Computer Engineering\u003c/p\u003e \u003ch2\u003eLab 5 Report\u003c/h2\u003e \u003cp\u003eECE 285-\u003c/p\u003e \u003ch2\u003eAlexander Ing\u003c/h2\u003e \u003ch2\u003eContents\u003c/h2\u003e \u003cp\u003e1 Thevenin’s Theorem 1 1.1 Theory and Calculations............................................ 1 1.2 Simulation.................................................... 2\u003c/p\u003e \u003cp\u003e2 Norton’s Theorem 4 2.1 Theory and Calculations............................................ 4 2.2 Simulation.................................................... 5\u003c/p\u003e \u003cp\u003e3 Conclusion 5\u003c/p\u003e \u003cp\u003eFigure 1.1: Circuit for Lab 5\u003c/p\u003e \u003cp\u003e1 Thevenin’s Theorem\u003c/p\u003e \u003ch2\u003e1.1 Theory and Calculations\u003c/h2\u003e \u003cp\u003eA. Find the theoretical Thevenin’s voltage VTh by finding the open-circuit voltage between terminals a and b for the circuit in Figure 1.1. Solution In order to find the theoretical Thevenin’s voltage VTh, we can use the redrawn circuit in Figure 1.2 and\u003c/p\u003e \u003cp\u003eFigure 1.2: Redrawn circuit from Figure 1.1 to find VTh\u003c/p\u003e \u003cp\u003efind the voltage at the terminals of R 3. The equivalent resistance in this circuit is expressed by summing the resistors R 1 , R 3 , and R 4 :\u003c/p\u003e \u003cp\u003eReq = 1 kΩ + 2.2 kΩ + 3 kΩ = 6.2 kΩ\u003c/p\u003e \u003cp\u003eThen, the current through the loop can be found by applying Ohm’s Law:\u003c/p\u003e \u003ch4\u003eI =\u003c/h4\u003e \u003ch4\u003eV\u003c/h4\u003e \u003ch4\u003eR\u003c/h4\u003e \u003ch4\u003e⇒ I =\u003c/h4\u003e \u003ch4\u003e10 V\u003c/h4\u003e \u003cp\u003eReq\u003c/p\u003e \u003cp\u003e≈ 1 .61 mA\u003c/p\u003e \u003cp\u003eLastly, we can apply Ohm’s Law again to find the voltage across this resistor.\u003c/p\u003e \u003cp\u003eVTh = IR 3 = (1.61 mA)(2.2 kΩ) ≈ 3 .55 V\u003c/p\u003e \u003cp\u003eB. Then find the theoretical Thevenin’s resistance RTh by removing the Load Resistor. Also replace the source V 1 with its internal resistance (ideally, a short). Solution To find the theoretical Thevenin’s resistance RTh, we can use the redrawn circuit in Figure 1.3 and solve for the equivalent resistance between terminals a and b.\u003c/p\u003e \u003cp\u003eRab ≡ RTh = R 2 + (R 3 ‖ (R 1 + R 4 )) + R 5 = 3 kΩ + (2.2 kΩ ‖ (1 kΩ + 3 kΩ)) + 10 kΩ ≈ 14 .4 kΩ\u003c/p\u003e \u003cp\u003e4 3\u003c/p\u003e \u003cp\u003e0\u003c/p\u003e \u003ch3\u003eTitle\u003c/h3\u003e \u003ch3\u003eSize\u003c/h3\u003e \u003ch3\u003eDate:\u003c/h3\u003e \u003ch3\u003eA\u003c/h3\u003e \u003ch3\u003eTitle\u003c/h3\u003e \u003ch3\u003eSize\u003c/h3\u003e \u003ch3\u003eDate:\u003c/h3\u003e \u003ch3\u003eA\u003c/h3\u003e \u003ch3\u003eTitle\u003c/h3\u003e \u003ch3\u003eSize\u003c/h3\u003e \u003ch3\u003eDate:\u003c/h3\u003e \u003ch3\u003eA\u003c/h3\u003e \u003ch3\u003eR_Th\u003c/h3\u003e \u003ch3\u003e14.4k\u003c/h3\u003e \u003ch3\u003e204 .0uA\u003c/h3\u003e \u003ch3\u003eV_Th\u003c/h3\u003e \u003ch3\u003e204 .0uA\u003c/h3\u003e \u003ch3\u003eLOAD\u003c/h3\u003e \u003ch3\u003e3k\u003c/h3\u003e \u003ch3\u003e204 .0uA\u003c/h3\u003e \u003ch3\u003e3.550V\u003c/h3\u003e \u003ch3\u003ea\u003c/h3\u003e \u003ch3\u003e612.1mV\u003c/h3\u003e \u003ch3\u003eb\u003c/h3\u003e \u003ch3\u003e0V\u003c/h3\u003e \u003cp\u003eFigure 1.5: Thevenin equivalent circuit simulation\u003c/p\u003e \u003cp\u003e4 3 2\u003c/p\u003e \u003ch4\u003eR\u003c/h4\u003e \u003cp\u003e3k\u003c/p\u003e \u003cp\u003e203 .7uA\u003c/p\u003e \u003ch4\u003eR\u003c/h4\u003e \u003cp\u003e2.2k\u003c/p\u003e \u003cp\u003e1.482mA\u003c/p\u003e \u003ch4\u003eR\u003c/h4\u003e \u003cp\u003e1k\u003c/p\u003e \u003cp\u003e1.685mA\u003c/p\u003e \u003ch4\u003eV\u003c/h4\u003e \u003cp\u003e1.685mA\u003c/p\u003e \u003ch4\u003eLOAD\u003c/h4\u003e \u003cp\u003e3k\u003c/p\u003e \u003cp\u003e203.7uA\u003c/p\u003e \u003ch4\u003eR\u003c/h4\u003e \u003cp\u003e10k\u003c/p\u003e \u003cp\u003e203.7uA\u003c/p\u003e \u003ch4\u003eR\u003c/h4\u003e \u003cp\u003e3k\u003c/p\u003e \u003cp\u003e1.685mA\u003c/p\u003e \u003ch4\u003e10.00V 8.315V\u003c/h4\u003e \u003cp\u003eb 0V 5.056V 7.093V\u003c/p\u003e \u003cp\u003ea 7.704V\u003c/p\u003e \u003cp\u003eFigure 1.6: Original circuit simulation\u003c/p\u003e \u003cp\u003e2 Norton’s Theorem\u003c/p\u003e \u003ch2\u003e2.1 Theory and Calculations\u003c/h2\u003e \u003cp\u003eA. Calculate the Norton’s resistance RN for the circuit in Figure 1.1. How is it related to Thevenin’s resistance RTh? Solution Norton’s equivalent resistance RN is calculated using the same process as RTh, thus it is the exact same. See part B from section 1.1 for the work.\u003c/p\u003e \u003cp\u003eRN ≡ RTh ≈ 14 .4 kΩ\u003c/p\u003e \u003cp\u003eB. Also calculate the Norton’s current IN for the circuit in Figure 1.1. Solution The Norton current IN can be calculated from our previously calculated values of VTh and RTh.\u003c/p\u003e \u003ch4\u003eIN =\u003c/h4\u003e \u003cp\u003eVTh RTh\u003c/p\u003e \u003ch4\u003e3 .55 V\u003c/h4\u003e \u003cp\u003e14 .4 kΩ\u003c/p\u003e \u003cp\u003e≈ 0 .247 mA\u003c/p\u003e \u003cp\u003eC. Draw the Norton’s equivalent circuit and calculate the voltage across the load resistor. Solution The Norton equivalent circuit is shown in Figure 2.1. As for the voltage across the load resistor, we must\u003c/p\u003e \u003cp\u003e4 3 2\u003c/p\u003e \u003cp\u003eTitle\u003c/p\u003e \u003cp\u003eSize Documen \u003cDoc\u003e\u003c/p\u003e \u003cp\u003e\u003cTitle\u003e\u003c/p\u003e \u003ch4\u003eA\u003c/h4\u003e \u003cp\u003eTitle\u003c/p\u003e \u003cp\u003eSize Documen \u003cDoc\u003e\u003c/p\u003e \u003cp\u003e\u003cTitle\u003e\u003c/p\u003e \u003ch4\u003eA\u003c/h4\u003e \u003cp\u003eTitle\u003c/p\u003e \u003cp\u003eSize Documen \u003cDoc\u003e\u003c/p\u003e \u003cp\u003e\u003cTitle\u003e\u003c/p\u003e \u003ch4\u003eA\u003c/h4\u003e \u003ch4\u003eI_N\u003c/h4\u003e \u003cp\u003e246.5u\u003c/p\u003e \u003ch4\u003eLOAD\u003c/h4\u003e \u003cp\u003e3k\u003c/p\u003e \u003ch4\u003eR_N\u003c/h4\u003e \u003cp\u003e14.4k\u003c/p\u003e \u003cp\u003eFigure 2.1: Norton equivalent circuit\u003c/p\u003e \u003cp\u003efirst calculate the equivalent resistance in the circuit.\u003c/p\u003e \u003cp\u003eReq = RN ‖ Rload =\u003c/p\u003e \u003cp\u003e14 .4 kΩ × 3 kΩ 14 .4 kΩ + 3 kΩ\u003c/p\u003e \u003cp\u003e≈ 2 .48 kΩ\u003c/p\u003e \u003cp\u003eNow, we can use Ohm’s Law to calculate the voltage across the parallel combination of everything.\u003c/p\u003e \u003cp\u003eV = IR ⇒ Vab = IN Req ≈ 611 mV\u003c/p\u003e ","relatedDocs":[{"id":8796451,"lang":"en","slug":"thevenin-norton-equivalent-circuits","title":"THEVENIN \u0026 NORTON EQUIVALENT CIRCUITS","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":7685862,"lang":"en","slug":"poly-mec-121-chapter-3-linear-and-angular-motion","title":"Thevenin and Norton Theorems: Simplifying Complex Circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":8796467,"lang":"en","slug":"experiment-4-thevenin-and-norton-equivalent-circuits","title":"experiment 4 thevenin and norton equivalent circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":8733508,"lang":"en","slug":"thestatutes-oftheuniversity-ofbath","title":"Finding Thevenin and Norton Equivalents in Electrical Circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":7050220,"lang":"en","slug":"electric-circuit-and-logic-gates-4","title":"Linear Circuits Analysis: Superposition, Thevenin/Norton Equivalent Circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":6774633,"lang":"en","slug":"practice-homework-11-introduction-to-electrical-engineering-ee-101","title":"EE101 Homework: Finding Thevenin and Norton Equivalent Circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":8891086,"lang":"en","slug":"nodal-analysis-1-thevenin-and-norton-equivalent-circuits","title":"Nodal Analysis 1 Thevenin and Norton equivalent circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":160972,"lang":"en","slug":"thevinin-and-norton-signal-and-system-assignment","title":"Finding Thevenin and Norton Equivalent Circuits for Given Circuits","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":8986135,"lang":"en","slug":"lecture-8-linearity-and-equivalent-circuits-i-v-thevenin","title":"Linearity and Equivalent Circuits: Finding Thevenin and Norton Equivalents","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":6512420,"lang":"en","slug":"thevenin-and-norton-equivalent-circuits-experiment-4-ee-302","title":"Thevenin and Norton Equivalent Circuits - Experiment 4 | EE 302","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":6397664,"lang":"en","slug":"notes-on-thevenin-and-norton-equivalent-circuits-ece-3710","title":"Notes on Thevenin and Norton Equivalent Circuits | ECE 3710","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0},{"id":291527,"lang":"en","slug":"maxpower-superposition-engineering-circuit-analysis-lecture-slides","title":"Maximum Power Transfer and Thevenin-Norton Equivalents","isStore":false,"isPrime":false,"isTop":false,"averageVotes":"0.0","reviewsCount":0}],"suggestedDocs":[]},"__N_SSP":true},"page":"/docs","query":{"slug":"lab-5-report-1","id":"8796475"},"buildId":"88ab84EjVlt2ImlLvPoah","assetPrefix":"https://assets.docsity.com/mf/docs/4.10.13","isFallback":false,"isExperimentalCompile":false,"gssp":true,"appGip":true,"locale":"en","locales":["default","it","en","es","pt","fr","pl","ru","sr","de"],"defaultLocale":"default","scriptLoader":[]}</script></body></html>
