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due 03/13 will include all instructions
– 2 years ago
**files (2)**
– ## SampleLabReport4.pdf
– PHYS1110Lab04-ElectricChargesandFields.pdf
**## SampleLabReport4.pdf**
Grade = 10/10
V. Good!
Lab Partners: Ainsworth Kiffin & Sammir Condezo Gonzales
Online Lab 7 – Resistors in Series and Parallel
University Name
PHYS 1110 – 01
21 March 2021
Dr. Nader Copty
Objectives:
The objective of this activity is to investigate the relationship between the equivalent resistance
and individual resistors connected in series and parallel. We will also investigate the voltage
across and current through resistors connected in series and parallel using simulation software.
Theory:
Before starting the experiment, there are a few concepts and equations that need to be known in
order to perform the lab:
β’A combination of resistors in a circuit can be replaced with an equivalent (total) resistor that
does not alter the circuit and has the same total current and potential difference as the actual
resistors.
β’The relationship between the current, voltage, and resistance is given by Ohmβs law:
π½ = π°πΉ
β’ Where:
o V = voltage or potential difference (V)
o I = current (A)
o R = resistance (β¦)
β’Resistors connected in series have the same current flowing through them. The equivalent
(total) resistance, current, and voltage of series combination are given by:
β’ πΉπ» = πΉπ + πΉπ + πΉπ +β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’Resistors connected in parallel have the same voltage applied across them. The equivalent
(total) resistance, current, and voltage of parallel combination are given by:
β’
π
πΉπ»
=
π
πΉπ
+
π
πΉπ
+
π
πΉπ
+β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’In this activity, we will simulate three resistors in various combinations in a circuit. We will
measure the current through the resistors, and the voltage cross the resistors.
β’We will determine the experimental value of the equivalent resistance (RT Exp) using Ohmβs
law and the accepted value of the equivalent resistance (RT Acc) using the given equations.
Equipment and Materials:
β’ Computer
β’ Scientific Calculator
β’ PhET Circuit Construction Kit: DC β Virtual Lab Simulation
[https://en.wikipedia.org/wiki/Graphing_calculator](https://en.wikipedia.org/wiki/Graphing_calculator)
[https://creativecommons.org/licenses/by-sa/3.0/](https://creativecommons.org/licenses/by-sa/3.0/)
Data:
β’ Part A- Resistor in Series
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 12.2 V I1 = 0.81 A
R2 V2 = 26.8 V I2 = 0.81 A
R3 V3 = 81.1 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 81.1 V I1 = 0.81 A
R2 V2 = 12.2 V I2 = 0.81 A
R3 V3 = 26.8 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81
β’ Part B- Resistor in Parallel
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 8.00 A
R2 V2 = 120.0 V I2 = 3.64 A
R3 V3 = 120.0 V I3 = 1.20 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 1.20 A
R2 V2 = 120.0 V I2 = 8.00 A
R3 V3 = 120.0 V I3 = 3.64 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Graphs:
Part A
Trial 1 Trial 2
Part B
Trial 1 Trial 2
Calculations:
Part A
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = V1 + V2 + V3
= 12.2 + 26.8 + 81.1
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 15.0 + 33.0 + 100.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = V1 + V2 + V3
= 81.1 + 12.2 + 26.8
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 100.0 + 15.0 + 33.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Part B
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 8.00 + 3.64 + 1.20
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/15.0) + (1/33.0) + (1/100.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 1.20 + 8.00 + 3.64
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/100.0) + (1/15.0) + (1/33.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Conclusions:
In Trial 1 of Part A, the total experiment voltage was 120.1 V. This resulted in a 0.08% error.
The total experimental current was calculated to be 0.81 A with a 0.00% error. The accepted
value of the total resistance was 148 β¦, which I successfully calculated with a 0.00% error. For
trial 2 we yielded the same results despite the same placement of each resistor. We yielded a
voltage of 120.1 V, an experimental current of 0.81 A and the total resistance of 148 β¦.
In Trial 1 of Part B, the total experiment voltage was 120.0 V. This resulted in a 0.00% error.
The total experimental current was calculated to be 12.8 A with a 0.00% error. The total
accepted resistance was calculated to be 9.35 β¦ while the total experimental resistance was
calculated to be 9.38 β¦, which I successfully calculated with a 0.32% error. For both trials we
yielded the same results despite the same placement of each resistor. So I conclude that the
position of the resistor doesnβt have any effect on the results as long as the values are the same in
each trial.
The final results obtained from the simulation do agree with the theory of this lab. The theory
stated that through Ohmβs Law voltage, the current is directly proportional to the voltage, and
inversely proportional to the resistance. When calculating our percent error for current and
resistance, it remained low, ranging from 0% – 2.21%. The low percent proved that the experiment
was accurate and precise. The placement and order of resistors has a great effect overall on all
parts of the experiment. Because they control the control of energy, similar to a dam, the remaining
electricity that can move throughout the system differs. This also depends on the strength of each
resistor.
Sources of Error:
The sources of error in this experiment maybe from:
β’ Inaccurate measurements of the voltmeter and ammeter.
β’ The quality of wires could greatly affect the measured conductivity.
β’ The uneven placement of the battery and resistors can also have an effect on the readings.
β’ The batteryβs output would affect the proper voltage to perform the lab.
References.
β’ Copty, Nader. βOnline Lab Experiment: Electric Charges and Fieldsβ Handout. Online
β’ Walker, Jearl, Robert Resnick, and David Halliday. Halliday & Resnick Fundamentals of
Physics. 11th ed. Hoboken, NJ: Wiley, 2018. Print.
β’ https://phet.colorado.edu/sims/html/circuit-construction-kit-dc-virtual-lab/latest/circuit-
construction-kit-dc-virtual-lab_en.html
Contributions:
Ainsworth Kiffin:
β’ Title Page
β’ Objective
β’ Theory Part A
β’ Equipment
β’ Part A: Data, Calculations and Graphs
β’ Part A: Analysis
Sammir Condezo Gonzales:
β’ Theory Part B
β’ Part B: Data, Calculations and Graphs
β’ Part B: Analysis
β’ Part A and B- Analysis
β’ Sources of Error
β’ References
**PHYS1110Lab04-ElectricChargesandFields.pdf**
This file is too large to display. [View in new window](https://www.sweetstudy.com/files/phys1110lab04-electricchargesandfields-pdf-10217757)
**PHYS1110Lab04-ElectricChargesandFields.pdf**
This file is too large to display. [View in new window](https://www.sweetstudy.com/files/phys1110lab04-electricchargesandfields-pdf-10217757)
**## SampleLabReport4.pdf**
Grade = 10/10
V. Good!
Lab Partners: Ainsworth Kiffin & Sammir Condezo Gonzales
Online Lab 7 – Resistors in Series and Parallel
University Name
PHYS 1110 – 01
21 March 2021
Dr. Nader Copty
Objectives:
The objective of this activity is to investigate the relationship between the equivalent resistance
and individual resistors connected in series and parallel. We will also investigate the voltage
across and current through resistors connected in series and parallel using simulation software.
Theory:
Before starting the experiment, there are a few concepts and equations that need to be known in
order to perform the lab:
β’A combination of resistors in a circuit can be replaced with an equivalent (total) resistor that
does not alter the circuit and has the same total current and potential difference as the actual
resistors.
β’The relationship between the current, voltage, and resistance is given by Ohmβs law:
π½ = π°πΉ
β’ Where:
o V = voltage or potential difference (V)
o I = current (A)
o R = resistance (β¦)
β’Resistors connected in series have the same current flowing through them. The equivalent
(total) resistance, current, and voltage of series combination are given by:
β’ πΉπ» = πΉπ + πΉπ + πΉπ +β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’Resistors connected in parallel have the same voltage applied across them. The equivalent
(total) resistance, current, and voltage of parallel combination are given by:
β’
π
πΉπ»
=
π
πΉπ
+
π
πΉπ
+
π
πΉπ
+β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’In this activity, we will simulate three resistors in various combinations in a circuit. We will
measure the current through the resistors, and the voltage cross the resistors.
β’We will determine the experimental value of the equivalent resistance (RT Exp) using Ohmβs
law and the accepted value of the equivalent resistance (RT Acc) using the given equations.
Equipment and Materials:
β’ Computer
β’ Scientific Calculator
β’ PhET Circuit Construction Kit: DC β Virtual Lab Simulation
[https://en.wikipedia.org/wiki/Graphing_calculator](https://en.wikipedia.org/wiki/Graphing_calculator)
[https://creativecommons.org/licenses/by-sa/3.0/](https://creativecommons.org/licenses/by-sa/3.0/)
Data:
β’ Part A- Resistor in Series
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 12.2 V I1 = 0.81 A
R2 V2 = 26.8 V I2 = 0.81 A
R3 V3 = 81.1 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 81.1 V I1 = 0.81 A
R2 V2 = 12.2 V I2 = 0.81 A
R3 V3 = 26.8 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81
β’ Part B- Resistor in Parallel
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 8.00 A
R2 V2 = 120.0 V I2 = 3.64 A
R3 V3 = 120.0 V I3 = 1.20 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 1.20 A
R2 V2 = 120.0 V I2 = 8.00 A
R3 V3 = 120.0 V I3 = 3.64 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Graphs:
Part A
Trial 1 Trial 2
Part B
Trial 1 Trial 2
Calculations:
Part A
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = V1 + V2 + V3
= 12.2 + 26.8 + 81.1
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 15.0 + 33.0 + 100.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = V1 + V2 + V3
= 81.1 + 12.2 + 26.8
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 100.0 + 15.0 + 33.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Part B
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 8.00 + 3.64 + 1.20
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/15.0) + (1/33.0) + (1/100.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 1.20 + 8.00 + 3.64
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/100.0) + (1/15.0) + (1/33.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Conclusions:
In Trial 1 of Part A, the total experiment voltage was 120.1 V. This resulted in a 0.08% error.
The total experimental current was calculated to be 0.81 A with a 0.00% error. The accepted
value of the total resistance was 148 β¦, which I successfully calculated with a 0.00% error. For
trial 2 we yielded the same results despite the same placement of each resistor. We yielded a
voltage of 120.1 V, an experimental current of 0.81 A and the total resistance of 148 β¦.
In Trial 1 of Part B, the total experiment voltage was 120.0 V. This resulted in a 0.00% error.
The total experimental current was calculated to be 12.8 A with a 0.00% error. The total
accepted resistance was calculated to be 9.35 β¦ while the total experimental resistance was
calculated to be 9.38 β¦, which I successfully calculated with a 0.32% error. For both trials we
yielded the same results despite the same placement of each resistor. So I conclude that the
position of the resistor doesnβt have any effect on the results as long as the values are the same in
each trial.
The final results obtained from the simulation do agree with the theory of this lab. The theory
stated that through Ohmβs Law voltage, the current is directly proportional to the voltage, and
inversely proportional to the resistance. When calculating our percent error for current and
resistance, it remained low, ranging from 0% – 2.21%. The low percent proved that the experiment
was accurate and precise. The placement and order of resistors has a great effect overall on all
parts of the experiment. Because they control the control of energy, similar to a dam, the remaining
electricity that can move throughout the system differs. This also depends on the strength of each
resistor.
Sources of Error:
The sources of error in this experiment maybe from:
β’ Inaccurate measurements of the voltmeter and ammeter.
β’ The quality of wires could greatly affect the measured conductivity.
β’ The uneven placement of the battery and resistors can also have an effect on the readings.
β’ The batteryβs output would affect the proper voltage to perform the lab.
References.
β’ Copty, Nader. βOnline Lab Experiment: Electric Charges and Fieldsβ Handout. Online
β’ Walker, Jearl, Robert Resnick, and David Halliday. Halliday & Resnick Fundamentals of
Physics. 11th ed. Hoboken, NJ: Wiley, 2018. Print.
β’ https://phet.colorado.edu/sims/html/circuit-construction-kit-dc-virtual-lab/latest/circuit-
construction-kit-dc-virtual-lab_en.html
Contributions:
Ainsworth Kiffin:
β’ Title Page
β’ Objective
β’ Theory Part A
β’ Equipment
β’ Part A: Data, Calculations and Graphs
β’ Part A: Analysis
Sammir Condezo Gonzales:
β’ Theory Part B
β’ Part B: Data, Calculations and Graphs
β’ Part B: Analysis
β’ Part A and B- Analysis
β’ Sources of Error
β’ References
**PHYS1110Lab04-ElectricChargesandFields.pdf**
This file is too large to display. [View in new window](https://www.sweetstudy.com/files/phys1110lab04-electricchargesandfields-pdf-10217757)
**## SampleLabReport4.pdf**
Grade = 10/10
V. Good!
Lab Partners: Ainsworth Kiffin & Sammir Condezo Gonzales
Online Lab 7 – Resistors in Series and Parallel
University Name
PHYS 1110 – 01
21 March 2021
Dr. Nader Copty
Objectives:
The objective of this activity is to investigate the relationship between the equivalent resistance
and individual resistors connected in series and parallel. We will also investigate the voltage
across and current through resistors connected in series and parallel using simulation software.
Theory:
Before starting the experiment, there are a few concepts and equations that need to be known in
order to perform the lab:
β’A combination of resistors in a circuit can be replaced with an equivalent (total) resistor that
does not alter the circuit and has the same total current and potential difference as the actual
resistors.
β’The relationship between the current, voltage, and resistance is given by Ohmβs law:
π½ = π°πΉ
β’ Where:
o V = voltage or potential difference (V)
o I = current (A)
o R = resistance (β¦)
β’Resistors connected in series have the same current flowing through them. The equivalent
(total) resistance, current, and voltage of series combination are given by:
β’ πΉπ» = πΉπ + πΉπ + πΉπ +β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’Resistors connected in parallel have the same voltage applied across them. The equivalent
(total) resistance, current, and voltage of parallel combination are given by:
β’
π
πΉπ»
=
π
πΉπ
+
π
πΉπ
+
π
πΉπ
+β―
β’ π°π» = π°π = π°π = π°π = β―
β’ π½π» = π½π + π½π + π½π +β―
β’In this activity, we will simulate three resistors in various combinations in a circuit. We will
measure the current through the resistors, and the voltage cross the resistors.
β’We will determine the experimental value of the equivalent resistance (RT Exp) using Ohmβs
law and the accepted value of the equivalent resistance (RT Acc) using the given equations.
Equipment and Materials:
β’ Computer
β’ Scientific Calculator
β’ PhET Circuit Construction Kit: DC β Virtual Lab Simulation
[https://en.wikipedia.org/wiki/Graphing_calculator](https://en.wikipedia.org/wiki/Graphing_calculator)
[https://creativecommons.org/licenses/by-sa/3.0/](https://creativecommons.org/licenses/by-sa/3.0/)
Data:
β’ Part A- Resistor in Series
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 12.2 V I1 = 0.81 A
R2 V2 = 26.8 V I2 = 0.81 A
R3 V3 = 81.1 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 81.1 V I1 = 0.81 A
R2 V2 = 12.2 V I2 = 0.81 A
R3 V3 = 26.8 V I3 = 0.81 A
Battery VT Acc
= 120.0 V IT Acc
= 0.81
β’ Part B- Resistor in Parallel
Trial 1: R1 = 15.0 β¦, R2 = 33.0 β¦, R3 = 100.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 8.00 A
R2 V2 = 120.0 V I2 = 3.64 A
R3 V3 = 120.0 V I3 = 1.20 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Trial 2: R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
Voltmeter & Ammeter
Across:
V (Volts) I (Amps)
R1 V1 = 120.0 V I1 = 1.20 A
R2 V2 = 120.0 V I2 = 8.00 A
R3 V3 = 120.0 V I3 = 3.64 A
Battery VT Acc
= 120.0 V IT Acc
= 12.8 A
Graphs:
Part A
Trial 1 Trial 2
Part B
Trial 1 Trial 2
Calculations:
Part A
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = V1 + V2 + V3
= 12.2 + 26.8 + 81.1
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 15.0 + 33.0 + 100.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = V1 + V2 + V3
= 81.1 + 12.2 + 26.8
= 120.1 V
% Error = ( (120 V – 120.1 V) / 120 V ) x 100% = 0.08%
IT Exp = (I1 + I2 + I3) / 3
= (0.81 + 0.81 + 0.81) / 3
= 0.81 A
% Error = ( (0.81 A – 0.81 A) / 0.81 A ) x 100% = 0.00%
RT Acc = R1 + R2 + R3
= 100.0 + 15.0 + 33.0
= 148 β¦
RT Exp = (VT Exp) / (IT Exp)
= (120.1 V) / (0.81 A)
= 148 β¦
% Error = ( (148 β¦ – 148 β¦) / 148 β¦ ) x 100% = 0.00%
Part B
Trial 1:
R1 = 15.0 β¦ R2 = 33.0 β¦ R3 = 100.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 8.00 + 3.64 + 1.20
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/15.0) + (1/33.0) + (1/100.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Trial 2:
R1 = 100.0 β¦, R2 = 15.0 β¦, R3 = 33.0 β¦
VT Exp = (V1 + V2 + V3) / 3
= (120.0 + 120.0 + 120.0) / 3
= 120.0 V
% Error = ( (120 V – 120 V) / 120 V ) x 100% = 0.00%
IT Exp = I1 + I2 + I3
= 1.20 + 8.00 + 3.64
= 12.8 A
% Error = ( (12.8 A – 12.8 A) / 12.8 A ) x 100% = 0.00%
RT Acc = 1 / (1/R1 + 1/R2 + 1/R3)
= 1 / ( (1/100.0) + (1/15.0) + (1/33.0))
= 9.35 β¦
RT Exp = (VT Exp) / (IT Exp)
= 120 V / 12.8 A
= 9.38 β¦
% Error = ( (9.35 β¦ – 9.38 β¦) / 9.35 β¦ ) x 100% = 0.32%
Conclusions:
In Trial 1 of Part A, the total experiment voltage was 120.1 V. This resulted in a 0.08% error.
The total experimental current was calculated to be 0.81 A with a 0.00% error. The accepted
value of the total resistance was 148 β¦, which I successfully calculated with a 0.00% error. For
trial 2 we yielded the same results despite the same placement of each resistor. We yielded a
voltage of 120.1 V, an experimental current of 0.81 A and the total resistance of 148 β¦.
In Trial 1 of Part B, the total experiment voltage was 120.0 V. This resulted in a 0.00% error.
The total experimental current was calculated to be 12.8 A with a 0.00% error. The total
accepted resistance was calculated to be 9.35 β¦ while the total experimental resistance was
calculated to be 9.38 β¦, which I successfully calculated with a 0.32% error. For both trials we
yielded the same results despite the same placement of each resistor. So I conclude that the
position of the resistor doesnβt have any effect on the results as long as the values are the same in
each trial.
The final results obtained from the simulation do agree with the theory of this lab. The theory
stated that through Ohmβs Law voltage, the current is directly proportional to the voltage, and
inversely proportional to the resistance. When calculating our percent error for current and
resistance, it remained low, ranging from 0% – 2.21%. The low percent proved that the experiment
was accurate and precise. The placement and order of resistors has a great effect overall on all
parts of the experiment. Because they control the control of energy, similar to a dam, the remaining
electricity that can move throughout the system differs. This also depends on the strength of each
resistor.
Sources of Error:
The sources of error in this experiment maybe from:
β’ Inaccurate measurements of the voltmeter and ammeter.
β’ The quality of wires could greatly affect the measured conductivity.
β’ The uneven placement of the battery and resistors can also have an effect on the readings.
β’ The batteryβs output would affect the proper voltage to perform the lab.
References.
β’ Copty, Nader. βOnline Lab Experiment: Electric Charges and Fieldsβ Handout. Online
β’ Walker, Jearl, Robert Resnick, and David Halliday. Halliday & Resnick Fundamentals of
Physics. 11th ed. Hoboken, NJ: Wiley, 2018. Print.
β’ https://phet.colorado.edu/sims/html/circuit-construction-kit-dc-virtual-lab/latest/circuit-
construction-kit-dc-virtual-lab_en.html
Contributions:
Ainsworth Kiffin:
β’ Title Page
β’ Objective
β’ Theory Part A
β’ Equipment
β’ Part A: Data, Calculations and Graphs
β’ Part A: Analysis
Sammir Condezo Gonzales:
β’ Theory Part B
β’ Part B: Data, Calculations and Graphs
β’ Part B: Analysis
β’ Part A and B- Analysis
β’ Sources of Error
β’ References
**PHYS1110Lab04-ElectricChargesandFields.pdf**
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