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CHM 2412 (Physical Chemistry Lab I)

schoolwork | Class … see also: 12th Grade – English / 4th Grade / CHM 1112 (General Chemistry Lab I) / PHY 1042 (General Physics Lab II) / 11th Grade – English – American Literature / BIO 1011 (Biology I: Cells)

Using a Parr Bomb to Measure Enthalpy

↘︎ Dec 9, 2008 … 3′ … download⇠ | skip ⇢

I. Introduction

The term enthalpy is used to describe the thermodynamic potential of a system. Heat of reaction, one form of enthalpy, is the energy given off by a substance upon combustion. It can be measured using a Parr bomb, which is an adiabatic container, held at a constant volume that ignites a substance. In this case, the heat of reaction is equal to the enthalpy because the reaction takes place at a constant volume and the change in pressure is negligible. The heat of reaction is also equal to the internal energy because of the constant pressure.

The substance to be measured is placed in the bomb, and the bomb is filled with oxygen and then sealed. The bomb is placed in a vessel of circulating water. The substance is ignited through wires touching it which are connected to a fuse box. The energy given off from combustion can then be measured from the changes in temperature of the water surrounding the bomb using a thermistor. The thermistor can be linked to a computer and the temperate as a function of time can be monitored and recorded. A substance of known enthalpy, or heat of reaction, is first used to create a constant for mass times Cp, so that a substance of unknown enthalpy can then be calculated from that information. The change in mass from each experimental run is negligible, making this method valid. The thermistor itself must also first be calibrated, by measuring a constant temperature bath and then changes in the temperature bath as a function of resistance.

II. Method

First, water that was a slightly above room temperature was placed in a vessel. The vessel was placed into the calorimeter and allowed to cool to room temperature. This change in temperature was measured and recorded with a thermistor and graphed on the computer as a function of resistance. This part of the experiment was performed without the actual bomb, as it was used for calibration purposes.

Next, the enthalpy of benzoic acid was measured. First, about 2000 g of water at room temperature was poured into the vessel. The exact weight of the water and vessel were recorded. Then a sample of about 1 g of benzoic acid was made into a pellet, and placed into the combustion cup. The exact weights of the benzoic acid pellet and combustion cup were also recorded. Fuse wire was attached to the electrodes, and it was made sure that the fuse wire securely touched the benzoic acid pellet. The lid of the bomb was securely attached, the bomb was purged with oxygen, and about 25 atmospheres of oxygen was pumped into the bomb.

The vessel was then placed into the calorimeter and bomb was placed into the vessel. The fuse connections were plugged into the bomb right before it was submerged in water. The lid of the calorimeter was placed on as to make sure the thermistor was in place in the water and so that the propeller could spin properly. The propeller was turned on and data was recorded on the computer. Once a stable temperature was reached, the bomb was ignited and again data was collected until a stable temperature was reached. This process was repeated for naphthalene and a food source (rice cakes).

III. Results

Water
Equation (x is resistance) y = -1E-08x3 + 4E-05x2 – 0.0811x + 348.34
Change in Temperature (K) 6.78183
Measurement Benzoic Acid Naphthalene Rice Cake
Weight of Water (g) 2005.60 1999.60 2030.00
Weight of Vessel (g) 782.96 784.70 —-
Weight of Combustion Cup (g) 13.8628 —- —-
Weight Pellet (g) 0.9488 0.9068 0.5097
Final Resistance 1041.37 1027.268 1190.49
Initial Resistance 1166.984 1200.926 1143.122
Final Temperature (K) 295.97 296.40 291.60
Initial Temperature (K) 292.28 291.31 292.96
Temperature Difference (K) 3.69 5.09 1.36
Theoretical q (kJ/g) 26.43 47.86 16.736
Theoretical q (kJ) 25.08 43.40 8.53
Actual q (kJ) —- 34.6 9.25
Percent Error —- 20.31% 8.44%
Rice Cake
Weight of Sample Rice Cake, hydrated (g) 3.1655
Weight of Sample Rice Cake, dry (g) 2.8013
Weight of Water in Hydrated Rice Cake (g) 0.3642

Calculations:

a. Heat capacity (mCp) from benzoic acid

qb.a. = 26.43 kJ/g (theoretical)

q = [mCp] ΔT
q = K ΔT

K = q / ΔT
K = (26.43 kJ/g) (0.9488 g) / (3.69 K)
K = 6.80 kJ / K

 

b. Heat of reaction of naphthalene and % error

qnap = 47.86 kJ/g (theoretical)
qnap = (47.86 kJ/g) x (0.9068 g)
qnap = 43.42 kJ

qnap = K ΔT
qnap = (6.80 kJ / K) x (5.09 K)
qnap = 34.6 kJ (actual)

Percent Error:
(34.6 kJ – 43.42 kJ) / 43.42 kJ x 100% = 20.31%

 

c. Heat of reaction of rice cake and % error.

16 Cal / 4 g (looked up) = x / 0.5097 g
x = 2.0388 Cal (for the 0.5097 g pellet)
2.0388 Cal x (4.184 kJ / Cal) = 8.53 kJ

qrice cake = 8.53 (theoretical)

qrice cake = (6.80 kJ / K) x (1.36 K)
qrice cake = 9.25 kJ (actual)

Percent Error:
(9.25 kJ – 8.53 kJ) / 8.53 kJ x 100% = 8.44%

 

IV. Conclusion

The difference in heat of reaction between the actual and theoretical values for naphthalene was 20.1%. The measured value was lower than the theoretical value. This means the change in water temperature was lower than it should have been. This error could have come from a few sources. The water used may have been warmer than room temperature, meaning that difference between the temperatures that the water was at and the temperature of room temperature water would have not been accounted for in the temperature difference. Another problem could have been that bomb was not flushed correctly with oxygen. This would cause an uneven ignition of the naphthalene, and the temperature might not have gone up as much as it should.

The difference in the heat of reaction between the actual and theoretical values for the rice cake was 8.44%. This seems like a fairly reasonable result. The actual value was high than that of the theoretical value. This could be accounted for in a few ways. The water used may have been colder than room temperature, causing a bigger change in temperature than there should have been. The bomb may also have been dirty, causing debris to ignite along with the rice cake, which would add to the temperature difference. The rice cake may also have gained some water vapor, causing water to ignite along with the rice cake, also causing a bigger change in temperature. Overall, the measured values as somewhat close to the theoretical values, showing there is some merit to the theories we have learned.

Me

circa 1996 (9 y/o)

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  • 08 Dec 9: Using a Parr Bomb to Measure Enthalpy #CHM 2412 (Physical Chemistry Lab I) #Dr. Jose Cerda #Saint Joseph's University
  • 08 Oct 6: Analysis of Ethanol and Butanol Solutions via Gas Chromatography #CHM 2412 (Physical Chemistry Lab I) #Dr. Jose Cerda #Saint Joseph's University

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Analysis of Ethanol and Butanol Solutions via Gas Chromatography

↘︎ Oct 6, 2008 … 3′ … download⇠ | skip ⇢

Introduction

During this laboratory experiment, a gas chromatograph was used to analyze the ethanol and butanol content of solutions of known mass ratios, and then construct a calibration curve using calculated area ratios from the graphs produced by the gas chromatograph. A solution of unknown mass ratio was then analyzed with the gas chromatograph in order to determine its area ratio. This area ratio was compared to the calibration curve in order to find the mass ratio of the unknown. Seven solutions of ethanol and butanol were prepared using different mass ratios of the two components. The solutions were then one by one injected into the gas chromatograph using a syringe. As each solution went through the gas chromatograph, the apparatus heated the solution. Ethanol and butanol have different chemical compositions and boiling points, so they reached a detector at different times. As the components reached the detector, the voltage given off by the components was read and recorded as a graph on a computer of time versus voltage.

Specifically, the gas chromatograph functions using an inert gas, in the case of this experiment, nitrogen, to function as a carrier gas for the analyte. The analyte is injected through a septum using a microsyringe. The carrier gas aids the analyte flow through the column. As the analyte moves through the column, the different components are separated and reach the detector at different rates, as the components have different chemical properties. In the case of this experiment, once the analyte reached the detector, the thermal conductivity of the components were measured as voltage. The voltage readings were graphed as a function of time on a computer.

Results

Desired Ratio of Masses of Ethanol to Butanol Mass of Ethanol (g) Mass of Butanol (g) True Ratio of Masses of Ethanol to Butanol Ratio of Areas of Ethanol to Butanol
1:7 1.0159 7.0125 0.14487 0.202332
2:6 1.9839 6.0561 0.327587 0.402598
3:5 3.0484 5.0139 0.60799 0.700423
4:4 4.0454 4.0669 0.994713 1.100032
5:3 5.0325 3.0001 1.677444 0.846482
6:2 6.2265 2.0196 3.083036 2.95128
7:1 7.0155 1.0104 6.94329 6.061587
Unknown 4.2861 2.7397 1.56441 1.559821*

*The graph of the original unknown was unreadable to determine the ratio of the areas, so

Anwar’s group’s graph of unknown was used to find a ratio of areas.

Equation of Linear Regression Line y = 1.134x – 0.0184
Mass Ratio of Unknown (Ethanol vs. Butanol) 1.750437
Substance Weight of Cut-out Piece of Paper for 4:4 Composition (g) Ratio of Areas
Ethanol 0.1121 1.094
Butanol 0.1025

Discussion and Conclusions

The calibration curve came out fairly well. It follows almost exactly a straight line except for the value where the ratio of masses was 5:3. The ratio of the areas is much lower than it should be. There is a decrease in the ratio of the areas from the 4:4 composition (1.100032), to the 5:3 composition (0.846482), and then the area ratio goes back up in the 6:2 composition (2.95128). The value for the ratio of the areas should have been somewhere between 1.100032 and 2.95128. Other than that one value, all the other values are very linear. It should have been expected that the values would linear, considering that the ratio of the masses was not increased exponentially; the ratios were only decreased and increased by a constant value. This also means the slope of the area ratio versus the mass ratio should be close to being in unity (a value of one), because of the constant increase and decrease in the mass ratio.

The ratio of the areas for the original unknown was unreadable on the graph, so another group’s unknown graph was used to find a ratio of areas. That group did not record their original masses used for their unknown sample, so it is not possible to find the percent error. However, using the equation for the linear regression line, the expected ratio of masses could be found by subbing the ratio of the areas in for “x”. The mass ratio found for their unknown was 1.750437, which is close to the mass ratio for the 5:3 composition (1.677444), so it can be estimated that their unknown was composed of about 5 grams of ethanol and 3 grams of butanol. A percent error can be determined by comparing one of the points on the calibration curve to the actual equation of the line. For example, using the 6:2 mass compisition, the actual mass ratio was 3.083036. However, using the calculated area, according to the calibration curve the theoretical mass ratio is 3.31701. This yields a percent error of 7.59%. This is a fairly low percent error, but it should be, as the linear regression line is calculated to make it as close to the points on the graph as possible.

Finally, using the alternative method of finding the ratio of areas by physically weighing the two curves, the value was extremely close to the calculated value. The calculated ratio for the 4:4 mass ratio was 1.100032, while the ratio from weighing the curves was 1.094. This shows that weighing all the curves would have been an acceptable way of determining the area ratios, rather than using the trapezoidal rule to calculate the area ratios. The trapezoidal rule has error to it, so weighing the curves may even be more accurate than using the trapezoidal rule. If it was not a requirement to use the trapezoidal rule, it would have been preferred to simply weigh all the curves, as this would have been a much quicker way of determining the area ratios.

Me

circa 2009 (21 y/o)

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ADAM CAP is an elastic waistband enthusiast, hammock admirer, and rare dingus collector hailing from Berwyn, Pennsylvania.

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