physics lab

need lab preformed and lab report. i have attached all information needed. Including a detailed sample lab report, which is exactly how the final report should look.

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– 1 –

Augusta Technical College

PHYS 1110L – Online Lab 3: Latent Heat of Fusion & Specific Heat

Objectives:

The purpose of this laboratory activity is to investigate the latent heat of fusion, specific heat,

thermal energy and the temperature of water and various metal objects. Experimental values

obtained from real data will then be compared to the accepted values. We will also explore the

various forms of energy and energy transfer using simulation software.

Equipment:

• Real data for Latent Heat of Fusion and Specific Heat (experiment previously performed)

• Scientific Calculator

• PhET Energy Forms and Changes Simulation Software

Theory:

• Latent heat of fusion for water ( Lf ) is the thermal energy ( Qf ) needed to melt one gram of

ice into water at temperature of zero degree Celsius (see below table for list of

accepted values):

𝑳𝒇 = 𝑸𝒇/𝒎 ⇒ 𝑸𝒇 = ±𝒎. 𝑳𝒇

Where: Lf = Latent heat of fusion, Qf = Thermal energy (heat), m = Mass of ice or water

• Specific heat of a metal object ( cmetal ) is the thermal energy ( QΔT ) that an object must absorb

or release to change its temperature ( ΔT ) by one degree Celsius (see below table for list of

accepted values):

𝒄𝒎𝒆𝒕𝒂𝒍 = 𝑸𝚫𝑻 /𝒎. 𝚫𝑻 ⇒ 𝑸𝚫𝑻 = 𝒄𝒎𝒆𝒕𝒂𝒍. 𝒎. 𝚫𝑻

Where: cmetal = Specific heat of metal, QΔT = Thermal energy (heat), m = Mass of metal,

ΔT = Temperature change of metal

• To determine the latent heat of fusion for water ( Lf ), we place ice in a calorimeter that contains

warm water. The ice starts at approximately 0 ºC, melts into water, and then warms up to the

same final temperature as the warm water. This thermal energy transferred to the ice is the same

as the thermal energy transferred from the initially warm water as it cooled down to the final

equilibrium temperature:

– 2 –

watericef

waterTiceTf

LostGain

LostGain

TcmTcmmL

Q

QQ

QQ

QQ

)()(

)( )(

|| ||

−=+

−=+

−=

=




ice

ificewater

wfwaterwater

f
m

)TT(mc)TT(mc
L

−−

=

Where: cwater = specific heat of water

mwater = mass of water

mice = mass of ice

Tw = initial temperature of warm water

Ti = initial temperature of ice ~ 0 oC

Tf = final equilibrium temperature of mixture

• To determine the specific heat of a metal ( cmetal ), we heat a metal and then place it in a

calorimeter that contains cool water. The metal starts at approximately 100 ºC, cools down, and

the cool water warms up to the same final equilibrium temperature. The thermal energy

transferred to the cool water is the same as the thermal energy transferred from the initially hot

metal as it cooled down to the final, equilibrium temperature:

metalwater

metalTwaterT

LostGain

LostGain

TcmTcm

QQ

QQ

QQ

)()(

)( )(

|| ||

−=

−=

−=

=



)(

)(

mfmetal

wfwaterwater

metal
TTm

TTmc
c

−−


=

Where: cwater = specific heat of water

mwater = mass of water

mmetal = mass of metal

Tw = initial temperature of cool water

Tm = initial temperature of hot metal ~ 100 oC

Tf = final equilibrium temperature of mixture

– 3 –

Part A – Latent Heat of Fusion:

• The experiment was previously performed, and the data was recorded using the above shown

apparatus setup for measuring the latent heat of fusion for water.

• Using a temperature sensor, the data collection program displayed the graph of Temperature

versus Time, as shown above.

• The calorimeter was half-filled with warm water of mass mwater, and few pieces of dried ice of

mass mice were added to the calorimeter while stirring the mixture. Mass values are recorded in

the below table.

• From graph of Temp versus Time, see above sketch, the values of the maximum (initial)

temperature of the warm water Tw and the minimum (final) temperature Tf were obtained and

recorded in the below table.

– 4 –

Part B – Specific Heat:

• The experiment was previously performed, and the data was recorded using the above shown

apparatus setup for measuring the specific heat of two metals.

• Using a temperature sensor, the data collection program displayed the graph of Temperature

versus Time, as shown above.

• A metal of mass mmetal was heated in in boiling water for at least 5 minutes (Tm ~ 100 oC ).

• The metal was then retrieved from the boiler, water on the metal was quickly shaken off, and

the metal was dropped it into the calorimeter that was half-filled with cool water of mass mwater.

Mass values are recorded in the below table.

• From graph of Temp versus Time, see above sketch, the values of the minimum (initial)

temperature of the cool water Tw and the maximum (final) equilibrium temperature Tf were

obtained and recorded in the below table.

– 5 –

Analysis:

• Part A – Latent Heat of Fusion:

1. The measured values of the various masses and temperatures are given in the below table.

2. Calculate the experimental latent heat of fusion for water (Lf ) using the equation in the theory

section and record the result in the below table.

3. Compare the experimental value to the accepted value given in the below tables by

calculating the % Error. Record value in the below table.

Percentage error is used to compare experimental (calculated) to accepted (true) values:

% Error = %100
||

A

EA
; Where: A = accepted value and E = experimental value.

4. How do the values compare and what factors do think may cause there to be a difference

between these values? Discuss

in your lab report.

5. Why do we dry the ice before dropping in the calorimeter?

Explain in your lab report.

6. Why did we not include the mass of the calorimeter (Styrofoam) in our calculations? Explain

in your lab report.

7. Derive in the theory section of your lab report the final equation for latent heat of fusion for

water (Lf ).

• Part B – Specific Heat:

1. The measured values of the various masses and temperatures are given in the below table.

2. Calculate the experimental specific heat of the two metals (cmetal) using the equation in the

theory section and record the results in the below table.

3. Compare the experimental values to the accepted values given in the below tables by

calculating the % Error. Record values in the below table.

Percentage error is used to compare experimental (calculated) to accepted (true) values:

% Error = %100
||

A

EA
; Where: A = accepted value and E = experimental value.

4. How do the values compare and what factors do think may cause there to be a difference

between these values? Discuss in your lab report

5. Why do we shake off any water on the metals before dropping them in the calorimeter?

Explain in your lab report.

– 6 –

6. Why did we not include the mass of the calorimeter (Styrofoam) in our calculations? Explain

in your lab report.

7. Derive in the theory section of your lab report the final equation for the specific heat of the

metals (cmetal).

Energy Forms and Changes Simulation:

• Explore the various types energy forms, phase changes, and temperature using the below PhET

Energy Forms and Changes Lab Simulation Software:

https://phet.colorado.edu/sims/html/energy-forms-and-changes/latest/energy-forms-and-

changes_en.html

Go to the “Intro” tab

> Drag 2 thermometers (upper left) to contact and measure the temperatures of the

“Iron cube” and “Water container”

> Drag “Iron cube” on top of a “Burner”

> Heat “Iron cube” by pulling up on burner temperature gauge and hold

> Observe thermometer temperature of cube increase

> Drag Iron cube and drop in “Water container”

> Observe two thermometer temperatures achieve equilibrium

> Repeat but now also heat/cool Water by dragging it on top of second burner

> Observe the effect on the two thermometer temperatures when they achieve equilibrium

> Repeat using “Brick cube” and/or “Olive Oil container”

> Observe the effect on the two thermometer temperatures achieve equilibrium

> Repeat by heating both Iron and Brick cubes on top of each other

> Observe thermometer temperatures of the two cubes increase

> Drag both cubes and drop in Water or Olive Oil container

> Observe the three thermometer temperatures achieve equilibrium

• Discuss observations and compare your lab and simulation results in your report conclusion.

• Save a screenshot (screen capture) of one trial of the energy forms and changes simulations to

include in the graphs section of your lab report

Lab Report:

• When writing the lab report, you must review and follow very carefully the Physics Lab Report

instructions and outline document.

• In your lab report, include the Title Page, Objectives, Theory, Equipment, Data, Graphs and

Screenshots, Calculations, Conclusions, Sources of Error, and References.

https://phet.colorado.edu/sims/html/energy-forms-and-changes/latest/energy-forms-and-changes_en.html

https://phet.colorado.edu/sims/html/energy-forms-and-changes/latest/energy-forms-and-changes_en.html

– 7 –

• Remember to show all equations and calculations in detail and to round the results to the correct

number significant digits and precision.

• In the conclusions section, be sure to summarize the final results, comment on the agreement

or disagreement of the results with the theory or expectations, answer analysis questions, and

discuss what you personally learned from this experiment and your observations/comments.

• Remember to also answer and discuss all analysis questions in your conclusions section.

• Submit your complete lab report electronically by the due date!

Tables of Accepted Values

Accepted Heat of Fusion Values

Substance cal/g kJ/kg

Water 79.5 333

Mercury 2.72 11.4

Hydrogen 13.9 58.0

Oxygen 3.32 13.9

Accepted Specific Heat Values

Substance cal/(g∙℃) J/(kg∙℃)

Zinc 0.092 390

Aluminum 0.21 900

Stainless Steel (Iron) 0.11 450

Copper 0.092 390

Brass 0.090 350

Ice 0.530 2220

Water 1.00 4187

Sea Water 0.93 3900

Styrofoam ~ 0.00 ~ 0.00

– 8 –

Physics – Online Lab: Latent Heat of Fusion and Specific Heat

Tables of Data and Results

• Part A – Latent Heat of Fusion:

Quantity Trial # 1 Trial # 2

Mass of water: mwater 249.0 g 212.0 g

Mass of ice: mice 52.0 g 16.0 g

Specific heat of water: cwater 1.00 cal/g∙℃ 1.00 cal/g∙℃

Initial temperature of warm water: Tw 28.4 °C 36.3 °C

Initial temperature of ice: Ti 0.00 ̊C 0.00 °C

Final equilibrium temperature of mixture: Tf 11.0 °C 28.5 °C

Accepted heat of fusion of water: Lf 79.5 cal/g 79.5 cal/g

Experimental heat of fusion of water: Lf (cal/g)

% Error

– 9 –

• Part B – Specific Heat:

Quantity Trial # 1 Trial # 2

Type of metal: Copper Brass

Mass of metal: mmetal 81.0 g 80.0 g

Mass of water: mwater 301.0 g 299.0 g

Specific heat of water: cwater 1.00 cal/g∙℃ 1.00 cal/g∙℃

Initial temperature of cool water: Tw 11.7 ̊C 15.0 ̊C

Initial temperature of hot metal: Tm 100.0 ̊C 100.0 ̊C

Final equilibrium temperature of mixture: Tf 13.9 ̊C 17.1 ̊C

Accepted Specific heat of metal: cmetal 0.092 cal/g∙C 0.090 cal/g∙C

Experimental Specific heat of metal: cmetal (cal/g∙C)

% Error

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:

•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.

•The relationship between the current, voltage, and resistance is given by Ohm’s law:

𝑽 = 𝑰𝑹

• Where:

o V = voltage or potential difference (V)

o I = current (A)

o R = resistance (Ω)

•Resistors connected in series have the same current flowing through them. The equivalent

(total) resistance, current, and voltage of series combination are given by:

• 𝑹𝑻 = 𝑹𝟏 + 𝑹𝟐 + 𝑹𝟑 +⋯

• 𝑰𝑻 = 𝑰𝟏 = 𝑰𝟐 = 𝑰𝟑 = ⋯

• 𝑽𝑻 = 𝑽𝟏 + 𝑽𝟐 + 𝑽𝟑 +⋯

•Resistors connected in parallel have the same voltage applied across them. The equivalent

(total) resistance, current, and voltage of parallel combination are given by:

𝟏

𝑹𝑻
=

𝟏

𝑹𝟏
+

𝟏

𝑹𝟐
+

𝟏

𝑹𝟑
+⋯

• 𝑰𝑻 = 𝑰𝟏 = 𝑰𝟐 = 𝑰𝟑 = ⋯

• 𝑽𝑻 = 𝑽𝟏 + 𝑽𝟐 + 𝑽𝟑 +⋯

•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.

•We will determine the experimental value of the equivalent resistance (RT Exp) using Ohm’s

law and the accepted value of the equivalent resistance (RT Acc) using the given equations.

Equipment and Materials:

• Computer

• Scientific Calculator

• PhET Circuit Construction Kit: DC – Virtual Lab Simulation

https://en.wikipedia.org/wiki/Graphing_calculator

https://creativecommons.org/licenses/by-sa/3.0/

Data:

• Part A- Resistor in Series

Trial 1: R1 = 15.0 Ω, R2 = 33.0 Ω, R3 = 100.0 Ω

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 Ω, R2 = 15.0 Ω, R3 = 33.0 Ω

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

• Part B- Resistor in Parallel

Trial 1: R1 = 15.0 Ω, R2 = 33.0 Ω, R3 = 100.0 Ω

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 Ω, R2 = 15.0 Ω, R3 = 33.0 Ω

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 Ω R2 = 33.0 Ω R3 = 100.0 Ω

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 Ω

RT Exp = (VT Exp) / (IT Exp)

= (120.1 V) / (0.81 A)

= 148 Ω

% Error = ( (148 Ω – 148 Ω) / 148 Ω ) x 100% = 0.00%

Trial 2:

R1 = 100.0 Ω, R2 = 15.0 Ω, R3 = 33.0 Ω

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 Ω

RT Exp = (VT Exp) / (IT Exp)

= (120.1 V) / (0.81 A)

= 148 Ω

% Error = ( (148 Ω – 148 Ω) / 148 Ω ) x 100% = 0.00%

Part B

Trial 1:

R1 = 15.0 Ω R2 = 33.0 Ω R3 = 100.0 Ω

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 Ω

RT Exp = (VT Exp) / (IT Exp)

= 120 V / 12.8 A

= 9.38 Ω

% Error = ( (9.35 Ω – 9.38 Ω) / 9.35 Ω ) x 100% = 0.32%

Trial 2:

R1 = 100.0 Ω, R2 = 15.0 Ω, R3 = 33.0 Ω

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 Ω

RT Exp = (VT Exp) / (IT Exp)

= 120 V / 12.8 A

= 9.38 Ω

% Error = ( (9.35 Ω – 9.38 Ω) / 9.35 Ω ) 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 Ω, 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 Ω.

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 Ω while the total experimental resistance was

calculated to be 9.38 Ω, 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 doesn’t 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 Ohm’s 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:

• Inaccurate measurements of the voltmeter and ammeter.

• The quality of wires could greatly affect the measured conductivity.

• The uneven placement of the battery and resistors can also have an effect on the readings.

• The battery’s output would affect the proper voltage to perform the lab.

References.

• Copty, Nader. “Online Lab Experiment: Electric Charges and Fields” Handout. Online

• Walker, Jearl, Robert Resnick, and David Halliday. Halliday & Resnick Fundamentals of

Physics. 11th ed. Hoboken, NJ: Wiley, 2018. Print.

• https://phet.colorado.edu/sims/html/circuit-construction-kit-dc-virtual-lab/latest/circuit-

construction-kit-dc-virtual-lab_en.html

Contributions:

Ainsworth Kiffin:

• Title Page

• Objective

• Theory Part A

• Equipment

• Part A: Data, Calculations and Graphs

• Part A: Analysis

Sammir Condezo Gonzales:

• Theory Part B

• Part B: Data, Calculations and Graphs

• Part B: Analysis

• Part A and B- Analysis

• Sources of Error

• References

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