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It is a lab report, To set up a circuit to verify Kirchhoff’s Voltage Law (KVL). KVL states that the algebraic sum of all the voltages around any closed loop in a circuit is equal to zero. This is because a circuit loop is a closed conducting path, so no energy is lost. It is basically, conservation of energy as moving around a closed loop.
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Submitted by: VADLAPUDI L S V RATNA CHOWDARY Roll No: 19CE
To set up a circuit to verify Kirchhoff’s Voltage Law (KVL).
KVL states that the algebraic sum of all the voltages around any closed loop in a circuit is equal to zero. This is because a circuit loop is a closed conducting path, so no energy is lost. It is basically, conservation of energy as moving around a closed loop. For Example, in the above circuit diagram R 1 , R2, R 3 are three resistors connected in series across a voltage source V. V 1 , V2, V 3 are the voltage drops across resistors R 1 , R2, R 3 respectively, and assuming that current is flowing in clock wise direction. So now according to Kirchhoff’s Voltage Law V + (-V 1 ) + (-V 2 ) + (-V 3 ) = V - V 1 - V 2 - V 3 = V = V 1 + V 2 + V 3
For the Loop A-B-C-D-E-A V(A) V(B) V(C) V(D) V(E) 10 4.08356 2.72238 1.36119 0 For the Loop B-F-E-D-C-B V(B) V(F) V(E) V(D) V(C) 4.08356 2.04178 0 1.36119 2. For the Loop A-B-F-E-A V(A) V(B) V(F) V(E) 10 4.08356 2.04178 0
For the Loop A-B-C-D-E-A V(AB) V(BC) V(CD) V(DE) V(EA) ALGEBRAIC SUM
From the above Experiment I got that Algebraic sum of Voltages for all the 3 Loops which are taken in the positive direction as “0”. This Indicates that the Kirchhoff’s Voltage Law (KVL) is Verified.
To set up a circuit to verify Kirchhoff’s Current Law (KCL).
Kirchhoff’s Current Law, often shortened to KCL, states that “The algebraic sum of all currents entering and exiting a junction must equal zero”. This is because it has no other place to go as no charge is lost. It is basically, conservation of charge entering and leaving a junction. From the above circuit, using KCL we can write, by assuming that currents away from the Junction as Positive. i 1 + (-i 2 ) + (-i 3 ) + i 4 = 0
Here all the currents are taken that they flow away from the Junction A, i.e. currents flowing away from junction are taken as positive.
According to KCL the algebraic sum of all currents entering and exiting a junction must equal zero. i.e. From the above circuit I(R 1 ) + I(R 2 ) + I(R 3 ) + I(R 4 ) + I(R 5 ) = 0 (-0.000732877) + 0.000821918 + 0.000821918 + 0.000821918 + (-0.00173288) ≈ 0 Note: Here even though I am using LT Spice stimulator (i.e. ideal situation) I didn’t get exact 0, because the decimals are exceeded the range of stimulator.
From the above experiment I came to know that the algebraic sum of all currents entering and exiting a junction must equal zero, i.e. charges entering and leaving the junction are being conserved, so finally the Kirchhoff’s Current Law is verified.
To find Current passing through a Resistor in the given circuit using Superposition Principle
For any linear and bilateral networks, consisting of two or more Independent Source (Voltage / Current Source), then current through (or voltage across) an element is the algebraic sum of the currents through (voltages across) that element caused by each independent source acting alone with all other sources are replaced by their internal resistances. i.e. replace the voltage sources with short circuit and replace the current source with the open circuit.
circuited the V 2 Voltage source, and the current is measured as I 2.
measured as IR3.
Now according to Superposition Principle, total current passing through R 3 is I 1 + I 2 , which is nothing but equal to IR
From this experiment I had calculated the current passing through R 3 Resistor using Superposition Theorem, and even I had calculated the current through normal method, and both methods gave same output. i.e. Superposition Theorem is verified.
First, measure the current through the path between points A and B (i.e. through R2). Note this as Iref (reference measurement).
Now, disconnect R2 from the circuit, i.e. there should be an open circuit in place of R2. And measure the voltage between points A and B. This gives the Thevenin’s voltage Vth. Now, deactivate the two voltage sources 5V and 10 V. Keeping R2 disconnected, measure the resistance between points A and B. This gives the Thevenin’s resistance Rth.
So now Ical = 0. And now Imeas, 1 is calculating the current passing through the resistor R 2 using the information of Thevenin’s equivalent Imeas, 1 = Vth / (Rth + R 2 ) = 5.87678 / ((1.270142878+5.7) * ( 3 )) = 0. Iref Ical Imeas, 1 Imeas, 2 0.000843136 0.0008431547647 0.0008431362316 0.
From the above Experiment I found that current passing through resistor R 2 is approximately 0.000843136, and by calculating the current value directly from the circuit gives the almost same value of current measured by Thevenin’s Theorem. So Thevenin’s Theorem is verified. And when I calculated the current through pen and paper, there is more deviation of current from the current measured through stimulator.