Kirchhoffs Rules Online Lab

Do you need this or any other assignment done for you from scratch?
We have qualified writers to help you.
We assure you a quality paper that is 100% free from plagiarism and AI.
You can choose either format of your choice ( Apa, Mla, Havard, Chicago, or any other)

NB: We do not resell your papers. Upon ordering, we do an original paper exclusively for you.

NB: All your data is kept safe from the public.

Click Here To Order Now!

Introduction

The aim of the experiment was to validate Kirchhoffs Rules as applied in electrical circuits. The practical work was undertaken virtually by using the PhET interactive simulation (PHET Interactive Simulations, 2021). The setup was designed and arranged as shown in the figure below. The lab work employed the general knowledge that distinct methods are utilized to study electronic circuits that are not reducible to simple parallel circuit sequences. The voltage differences and currents across the resistors cannot be examined by applying the general Ohms Law. Points D and A are referred to as junctions as at least two wires intersect there.

A closed-loop comprises any path that commences at a particular point in the circuit, flows through the circuits elements, and returns to the same initial position. From the figure, the three closed loops are A-B-C-D-A, A-D-E-F-G-A, and B-C-D-E-F-G-A-B. The loops and junctions are employed to study the circuit using the two Kirchhoffs laws, namely the Kirchhoffs Current Rule (KCR) and Kirchhoffs Voltage Rule (KVR). KCR stipulates that the summation of currents flowing into the junction is equal to the sum of currents from the intersection. KVR states that the algebraic sum of the voltage drops within any confined loop is equivalent to zero.

Kirchhoffs Rules Online Lab

Labeling and arbitrarily assigning current flow directions on every circuit portion, the junction equation at D yields: l1 + l3  l2 = 0  (I)

Traversing the closed loops in random directions and setting all the voltage changes to zero, the equivalent equation becomes: £ ”V = 0 (II)

Where Ohms Law gives the voltage difference across the resistance (V) expressed as: ”V = IR  (III)

From the preceding expressions, the equations for the three loops can be represented as follows:

Loop A-B-C-D-A with A as the commencing point and assuming clockwise flow: V1  I1R1  I1R2  I3R3 = 0 (IV)

Loop A-D-E-F-G-A with A as the starting point and a clockwise flow:  I3R3  I2R1 + V2  I2R5 = 0 (V)

Loop B-C-D-E-F-G-A-B, which is a dependent equation derived from the summation of equations (iv) and (v), yields: + V1  I1R1  I1R2  I2R2 + V2  I2R5 = 0 (C)

Theoretically, the solutions for the unknown currents ( I1, I2, I3) in the simultaneous equations are achieved by solving equation (I) and two other equations picked from equations (IV), (V), and (V). The negative current attained from computations implies that the current was flowing in the opposite direction from the arbitrarily assigned direction.

Procedure

  • Five resistors labeled: R1, R2, R3, R4 ‘ R5, with resistances of 10©, 15©, 20©, 25© and 30©, respectively, were selected.
  • The resistors were arranged and connected on the PhET simulation forming the initially shown circuit diagram. Two batteries of voltages V1 and V2 measuring 7.5V and 9.0V, respectively, were fixed in their designated points of the circuit. The resistors R1, R2, R3, R4 ‘ R5 were also attached to their appropriate positions in the circuit. With the complete setup, the potential differences across the batteries were measured using a voltmeter and recorded as V1 and V2.
  • The currents I1, I2, I3 were computed by employing the two Kirchhoffs Rules and the known battery voltages and resistances. The worked-out currents were used in Ohms Law for the calculation of the voltage drops across every resistor. During computation, equivalent current directions and notation were utilized as depicted in the schematic diagram.
  • With the theoretical figures rough idea, the potential difference across each resistor was afterward measured and recorded.
  • The readings of the main currents I1, I2, I3 were then made using an ammeter. This was achieved by snapping the circuit and inserting the ammeter in series with the loop wires.
  • Finally, the deviations between the computed and weighted figures of the voltages and currents were calculated, and the percentage errors were derived. Verification of the loop rules and Kirchhoffs laws was also done.

Data Observations

Measured Voltages V1 and V2

V1 = 7.5 V
V2 = 9.0 V

Measured Currents and Voltages across Resistors

Resistance (©) Measured Current (A) Measured Voltage
R1 = 10 0.25 2.50
R2 =15 0.25 3.74
R3 =20 0.06 1.26
R4 =25 0.19 4.66
R5 =30 0.19 5.60

Measured Currents I1, I2, I3

I1 = 0.25

I2 = 0.19

I3 = 0.06

Data Analysis/ Calculations

Theoretical Calculation of  I1, I2, I3

  • From equation (I) l1 = l2 + l3
  • Substituting the values of resistors into equation (IV) yields

    • 7.5  10I1  15I1 + 20I3 = 0
    • 25I1  20I3 = 7.5
  • Substituting the resistors figures into expression (V) yields

    • 20I3  25I2 + 9  30I2 = 0
    • 55I2 + 20I3 = 9
  • Replacing I2 in equation (VII) into equation (IX) yields

    • 55(I1 + I3) + 20I3 = 9
    • 55 I1 + 75I3 = 9
  • Solving equations (VIII) and (X) simultaneously yields

    • 55(25I1 + 20I3) = 7.5
    • 25 (55I1 + 75I3) = 9
    • -2975 I3 = 187.5
    • I3 = 187.5/-2975 = -0.06 A
  • From equation (VIII), I1 = 7.5 + 20I3/ 25 = 7.5 + 20(-0.06)/25 = 6.3/25 = 0.25A
  • From equation (VII), I2 = I1 + I3 = 0.25 + (-0.06) = 0.19A

Verifying Kirchhoffs and Loops Rules

  • From I1 + I3  I2 = 0
  • 0.25 + (-0.06)  0.19 = 0
  • 0=0

From loop A-B-C-D-A equation (one of the loops)

  • V1  I1R1  I1R2 + I3R3 = 0
  • 7.5 + 0.25 (10)  0.25 (15) + (-0.06)(20)
  • 7.5  2.5  3.75  1.2 = 0
  • 0.05 = 0
  • 0=0

Potential Differences across Resistors

Vr1 = I1 x R1 = 0.25 x 10 = 2.50 V

Vr2 = I1 x R2 = 0.25 x 15 = 3.75 V

Vr3 = I3 x R3 = 0.06 x 20 = 1.20 V

Vr4 = I2 x R1 = 0.19 x 25 = 4.75 V

Vr5 = I2 x R5 = 0.19 x 30 = 5.70 V

Data Comparison and Percentage Errors

Resistance Current (A) Voltage (V)
Calculated
A
Measured
B
% Error
(A-B/A x 100)
Calculated
C
Measured
D
% Error
(C-D/C x 100)
R1= 10 0.25 0.25 0.00 2.50 2.50 0.00
R2=15 0.25 0.25 0.00 3.75 3.74 0.27
R3=20 0.06 0.06 0.00 1.20 1.26 5.00
R4=25 0.19 0.19 0.00 4.75 4.66 1.89
R5=30 0.19 0.19 0.00 5.70 5.60 1.75

Conclusion

From the data analysis, it was observed that the computed value of I3, was negative, suggesting that the current flow was counter-clockwise in the assumed direction. The measured and calculated values of currents across individual resistors did not vary since the primary current remained constant. Further, percentage errors between the measured and calculated voltages were minimal due to a lack of active human involvement. Nevertheless, the virtual lab was a success as Kirchhoffs Rule and loop rule were demonstrated and verified.

Reference

PHET Interactive Simulations (2021). Circuit construction kit: Dc  virtual lab.

Do you need this or any other assignment done for you from scratch?
We have qualified writers to help you.
We assure you a quality paper that is 100% free from plagiarism and AI.
You can choose either format of your choice ( Apa, Mla, Havard, Chicago, or any other)

NB: We do not resell your papers. Upon ordering, we do an original paper exclusively for you.

NB: All your data is kept safe from the public.

Click Here To Order Now!