DC Circuits Lab Template (Revised) (1) (2)

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Mt San Antonio College *

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211

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Physics

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Apr 3, 2024

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7

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Title of the Experiment: DC Circuits Lab Student’s name: Jesus Gonzalez Section SLN:13710 TA’s Name: Sang-Eon Week of the experiment: 4 1
OBJECTIVE ( 3 points ): The objective of the lab is to apply Ohms Law, test kirchhoff’s voltage and current laws in simulated circuit, and fine the condition for max power transfer from source voltage to load. EXPERIMENTAL DATA & DATA ANALYSIS & RESULTS PART I. Ohm’s Law. A. Determining the resistance of a pencil lead. Figure 1: Pencil Circuit Internal battery resistance R = 9 ( Ω ) V battery (V) 20 40 60 80 100 I PENCIL (A) .59 1.18 1.76 2.35 2.94 V PENCIL (V) 14.71 29.41 44.12 58.82 73.53 2
Figure 2: Logger Pro (V, I) m (slope) = .040 R; Δ m = 24.99 R R = 1/m = 1/.40 = 25R ; Δ R = 1/24.99 = .40R R mean = 24.99 ; % diff = |(25-24.99)/25|*100 = .04% - Based on your data conclude whether the virtual pencil was an ohmic element or not. B. Virtual pencil lead (VP) ρ = 4.2*10^-4 ( Ω∙m ); R VP = 25 Ω D = 0 .6( mm ); Area = piR^2= .2827m^2 L =R*A/P ( m ) = C. Real pencil rod (RP) ρ = 4.2*10^-4( Ω∙m ); D ± ΔD = 2.4 ± .01 ( mm ); L± ΔL = 18 ± 0.1 ( cm ); R RP = 4.2*10^-4(18/pi(0.0024^2) = 4.17 Ω (unit); ∆ R RP = 2.4+0.1 = 12.91 Ω (unit) 3
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If you assume that the virtual pencil lead was made out of material of resistivity ρ = 3.5×10-4 Ω∙m (a composition of graphite) and the diameter of the lead was 0.6 mm, how long was the pencil? On average the real pencil rod has a diameter of 2.4 ± 0.1 mm and the length of 18.0 ± 0.1 cm. If it was made of the same material as the virtual pencil what resistance would it have? R=PL/A 3.54*10^-4*18*10^-2/4.42*10^-6 = 13.94Ω R*A/P = 1.126cm PART II-1. Kirchhoff’s Rules V 1 = 10 (Volts); V 2 = 18 (Volts); R 1 =15 (Ω); R 2 = 8 (Ω); R 3 = 25 (Ω); Figure 3: Kirchhoff’s Rules with Ammeters and Voltmeters Junction A: I = 1.12 A .27 A 1.40 A = 0 Junction B: I = 1.40 A + .27 A 1.12 A = 0 Loop 1: V = ( ε IR )= ¿¿ 10 + 0I - 10I = 0 Loop 2: V = ( ε IR )= 10 + .27 I .27 I = 0 4
Did the currents for junctions A and B add up to zero? Yes Did the voltages around loop 1 and loop 2 add up to zero? Yes, both rules applied here as expected PART II-2. Electric Power Figure 4 : Power Transfer Circuit Figure 5: Power vs. Load Resistance 5
V emf ( ε battery ) = 8V ( Volts ); Internal resistance R S =4 ( Ω ); R Load (Ω) 1 2 3 4 5 6 7 8 9 10 20 30 40 50 60 I (A) 1.6 1.3 3 1.1 4 1 .89 .80 .73 .67 .62 .57 .33 .24 .18 .15 .13 V Load (V) 1.6 2.6 7 3.4 3 4 4.4 4 4.8 5.9 5.3 3 5.5 4 5.71 6.67 7.06 7.27 7.41 7.5 A = 66.44 (unit); B = 4.098 (unit); ε = = 8.15 V ; % error of ε (with ε battery = 8 V) =1.875% From your fit what value of R L maximizes the power in the load? How does it compare to our simulated internal resistance of the battery set to R S = 7 Ω? The internal resistance of the battery is 10Ω The load resistance that maximizes the power in R L = B = 4 ( Ω ) % error of R L (with R S = 4 Ω) = 0% Derivation of the condition for a maximum power transfer in a simple DC Circuit .P=I^2R_L dP/dR_L = v_th^2* DISCUSSION & CONCLUSION ( 10 points ): The objective of this lab was to apply Ohms Law, test kirchhoff’s voltage and current laws in simulated circuit, and fine the condition for max power transfer from source voltage to load. This was accomplished by analyzing simulated circuits with resistors and voltage sources using voltmeters and ammeters to test and verify voltages and currents and use Kirchhoff's rules and Ohm Laws to verify each current, voltage drop and resistance. In part 1 of the lab we used the lead of a pencil and measured the voltage and resistance across the pencil in series. In logger pro we notice that as voltage increases, resistance slowly increases as well, also you need a large increase in Voltage for a decent current increase. Based on the data calculated resistance on the graph is similar to that simulated. 6
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In part 2 with the kirchhoffs rules we do circuit analysis across resistors using the loop rule to find currents and voltage drops. The rule is that current cant be stored in any node and voltage out is equal to voltage in so the drop is always equal to 0 and the current at any node is 0. In the power transfer circuit we recognize in the data that as current decreases the voltage on the load increases as well as resistance. In conclusion we became familiar with ohms law and kirchhoffs rules. Upon doing the simulations we were able to visualize the flow of electrons, voltage and how resistance acts upon each unit using V=IR. 7