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PChem Experiment No. 1
The thermodynamics of a galvanic cell
1. Aims
The experiment aims to verify the validity of the Nernst equation, ๐ธ๐‘Ž = ๐ธ๐‘Ž0 +
๐‘…๐‘‡
๐‘Ž
๐‘…๐‘‡
0
ln(๐‘Ž ๐‘œ๐‘ฅ )for the EMF of a half cell and ๐ธ๐‘๐‘’๐‘™๐‘™ = ๐ธ๐‘๐‘’๐‘™๐‘™
+ ๐‘›๐น ln(๐‘„) for a full galvanic cell.
๐‘›๐น
๐‘Ÿ๐‘’๐‘‘
The experiment also aims to find values for ฮ”S0,ฮ”H0,ฮ”G0 from the verified Nernst
equations for the cell.
2. Introduction
A Galvanic cell produces a flow of charge across a wire between two half cells due
to separate oxidation and reduction reactions taking place in each half cell. The
anode of the cell consists of a zinc rid immersed in ZnSo4. The metal is oxidized
according to the equation
๐‘ฆ๐‘–๐‘’๐‘™๐‘‘๐‘ 
๐‘๐‘› (๐‘ ) โ†’
๐‘๐‘›2+ (๐‘Ž๐‘ž) + 2๐‘’ โˆ’
The cathode consists of a platinum electrode in a mixture of 0.2M potassium
ferrocyanide and 0.2M potassium ferricyanide, the relative ratios of which determine
the EMF produced by the half-cell. The potassium ferricyanide is reduced according
to the equation
๐‘ฆ๐‘–๐‘’๐‘™๐‘‘๐‘ 
[๐น๐‘’(๐ถ๐‘)6 ]3โˆ’ + ๐‘’ โˆ’ โ†’
[๐น๐‘’(๐ถ๐‘)6 ]4โˆ’
Using the Nernst equation, the EMF produced by half cell containing the cathode is
given by:
๐ธ๐‘Ž = ๐ธ๐‘Ž0 +
๐‘…๐‘‡ [๐น๐‘’ 3+ ]
ln(
)
๐‘›๐น [๐น๐‘’ 2+ ]
The EMF produced by the whole cell is given by:
0
๐ธ๐‘๐‘’๐‘™๐‘™ = ๐ธ๐‘๐‘’๐‘™๐‘™
+
๐‘…๐‘‡ [๐น๐‘’ 3+ ]
ln(
)
๐‘›๐น [๐น๐‘’ 2+ ]
In the first part of the experiment the EMF is measured for a range of ratios of
ferricyanide to ferrocyanide(1:1, 10:1, 1:10) and the data is used to verify the Nernst
Equations above. The second part of the experiment measures a the EMF across
the cell for a series of temperatures while the ferri:ferro remains constant at 1:1. EMF
is then plotted as a function of temperature. Then using the equation
๐›ฅ๐‘† 0 = ๐‘›๐น(
0
๐‘‘๐ธ๐‘๐‘’๐‘™๐‘™
)
๐‘‘๐‘‡ ๐‘ƒ
๐›ฅ๐‘† 0 may be determined. ๐›ฅ๐บ 0 can be determined from the equation
0
๐›ฅ๐บ 0 = โˆ’๐‘›๐น๐ธ๐‘๐‘’๐‘™๐‘™
Then using the attained values for ๐›ฅ๐บ 0 and ๐›ฅ๐‘† 0 , ๐›ฅ๐ป 0 can be determined from the
equation
๐›ฅ๐บ 0 = ๐›ฅ๐ป 0 โˆ’ ๐‘‡ ๐›ฅ๐‘† 0
3. Experimental Procedure
Part I
100cm3 of 0.2M potassium ferricyanide solution was prepared. The zinc electrode
was rinsed in dilute nitric acid solution and then rinsed with deionized water. The cell
was assembled and was then placed in a two liter beaker filled with water at room
temperature. 10cm3 of 1M ZnSO4 was added to the zinc half-cell. Using the
potassium ferrocyanide solution provided, 10cm3 of a 1:1 mixture of ferrocyanide and
ferricyanide was prepared and added to the other half cell. The electrodes were
connected to the potentiometer and the cell was made sure to be in thermal
equilibrium. The temperature of the cell was then recorded to be 294.5 oK. The EMF
produced by the cell was recorded and then recorded again for
ferrocyanide:ferricyanide ratios of 10:1 and 1:10 respectively.
Part II
A mixture of ferrocyanide:ferricyanide of 1:1 was placed in the half-cell containing the
Pt electrode. The assembly was placed in the two liter beaker, which contained an
ice-water mixture, with a thermometer in the half-cell containing the Pt electrode. At
thermal equilibrium the temperature and the EMF across the cell were recorded.
The water/ice mixture was then replaced with water at room temperature. The
beaker was then placed on a hot-plate with a temperature control. Stirring the water
to maintain thermal equilibrium between half-cells, the cell was heated over a
temperature range from 275.65oK to 333.15oK and at 5oK intervals the EMF and
temperature were recorded.
4. Results
Part I
The EMFs were recorded with the varied ratios of ferrocyanide to ferricyanide as
follows.
EMF(V)
Ferro:ferri ratio
1.246
1:1
1.173
1:10
1.273
10:1
[๐น๐‘’ 3+ ]
Then, the EMF was plotted as a function of ln([๐น๐‘’ 2+]).
EMF vs. ln(aox/ared)
1.3
1.28
E
1.26
c
e
l
l
1.24
Series1
1.22
(
Linear (Series1)
1.2
V
)
1.18
1.16
-4
-2
0
2
ln(aox/ared)
4
y = mx + c
R² = 0.9341
m=0.0217
C=1.2307
The results confirm Nernstโ€™s equation in that they demonstrate a linear correlation
[๐น๐‘’ 3+ ]
between Ecell and ln([๐น๐‘’ 2+]), which is outlined in the form of the Nernst equation:
0
๐ธ๐‘๐‘’๐‘™๐‘™ = ๐ธ๐‘๐‘’๐‘™๐‘™
+
๐‘…๐‘‡ [๐น๐‘’ 3+ ]
ln(
)
๐‘›๐น [๐น๐‘’ 2+ ]
In the diagram above m correlates to
๐‘…๐‘‡
๐‘›๐น
0
0
and C, the intercept, is ๐ธ๐‘๐‘’๐‘™๐‘™
. Hence ๐ธ๐‘๐‘’๐‘™๐‘™
was
found to be 1.2307V. To calculate the value of the standard Gibbโ€™s energy for the cell
it was necessary to calculate a value of nF where n=1 and
F=96,485.3365(21) C/mol.
0
๐›ฅ๐บ 0 = โˆ’๐‘›๐น๐ธ๐‘๐‘’๐‘™๐‘™
๐›ฅ๐บ 0 was found to be -237489.0072Jmol-1.
๏ƒ  Do your results confirm Nernstโ€™s equation? Discuss whether this is the case and
explain how you reached your conclusions.
๏ƒ  Obtain the best linear fit of your plot and use slope and intercept to determine the
cell standard potential E0 and the ๏„G0 of the redox reaction taking place in the cell.
Part II
The values of EMF changed with temperature as follows.
Temp(oK)
EMF(V)
275.65
1.211
288.15
1.193
293.15
1.188
298.15
1.183
303.15
1.177
308.15
1.172
313.15
1.167
318.15
1.161
323.15
1.154
328.15
1.146
333.15
1.137
๐ธ๐‘๐‘’๐‘™๐‘™ =
0
๐ธ๐‘๐‘’๐‘™๐‘™
๐‘…๐‘‡ [๐น๐‘’ 3+ ]
+
ln(
)
๐‘›๐น [๐น๐‘’ 2+ ]
0
The ratios of oxidant to reductant is 1:1 and as ln(1) is equal to zero, ๐ธ๐‘๐‘’๐‘™๐‘™ = ๐ธ๐‘๐‘’๐‘™๐‘™
because the rest of the equation above becomes zero.
EMF vs. temperature
1.22
1.21
1.2
E 1.19
c
e 1.18
l 1.17
l
1.16
V
1.15
1.14
1.13
Series1
Linear (Series1)
(
y = -0.0012x + 1.5458
R² = 0.9932
)
0
100
200
300
400
temperature(หšK)
(
0
๐‘‘๐ธ๐‘๐‘’๐‘™๐‘™
๐‘‘๐‘‡
)๐‘ƒ can be taken to equal the slope of the plot above. By combining the
equations
๐›ฅ๐บ 0 = ๐›ฅ๐ป 0 โˆ’ ๐‘‡ ๐›ฅ๐‘† 0
And
0
๐›ฅ๐บ 0 = โˆ’๐‘›๐น๐ธ๐‘๐‘’๐‘™๐‘™
,
And assuming that ๐›ฅ๐ป 0 is negligible, ๐›ฅ๐‘† 0 is given by
0
๐‘‘๐ธ๐‘๐‘’๐‘™๐‘™
๐›ฅ๐‘† = ๐‘›๐น(
)
๐‘‘๐‘‡ ๐‘ƒ
0
Using this equation the value of ๐›ฅ๐‘† 0 was calculated to be -231.5648JK-1. ๐›ฅH 0 was
then be calculated using the value for ๐›ฅ๐บ 0 calculated in part 1, the temperature,
T,(294.5oK) from the equation
๐›ฅ๐บ 0 = ๐›ฅ๐ป 0 โˆ’ ๐‘‡ ๐›ฅ๐‘† 0
๐›ฅH 0 was found to be -169293.1736J.
.
5. Discussion and Conclusions
[๐น๐‘’ 3+ ]
The linear relationship of Ecell and ln([๐น๐‘’ 2+]) shown in the graph of the data acquired
from part 1 of the experiment verified the Nernst equation for a galvanic cell. From
the intercept of the plot, Ecell was evaluated to be 1.2307V and from this value the
Gibbsโ€™ free energy was calculated to be -138871.2808Jmol-1.
๐‘ฆ๐‘–๐‘’๐‘™๐‘‘๐‘ 
The standard potential for the reaction ๐‘๐‘›(๐‘ ) โ†’
๐‘๐‘›2+ (๐‘Ž๐‘ž) + 2๐‘’ โˆ’ is given as
0.7618volts (see Vanýsek, Petr (2007). โ€œElectrochemical Seriesโ€, in Handbook of
Chemistry and Physics: 88th Edition) and for the reaction
๐‘ฆ๐‘–๐‘’๐‘™๐‘‘๐‘ 
[๐น๐‘’(๐ถ๐‘)6 ]3โˆ’ + ๐‘’ โˆ’ โ†’
[๐น๐‘’(๐ถ๐‘)6 ]4โˆ’ it is given as 0.361V(Atkins, P. de Paula J.
(2010). Atkin's Physical chemistry. Oxford. W.H Freeman and company. Ninth
edition. p928. )(both at 298.15oK). Hence the standard potential reference value
for our cell was 1.1228V.By substituting the temperature value of 298.15oK
into the equation for our plot of the change in standard potential with respect
to temperature, the value for standard potential at 298.15oK was
experimentally found to be 1.18802V. This left a discrepancy of 0.065V
between the reference value and that obtained through experiment.
Summarize your findings and results. Compare your standard potential results to
those you can calculate from reference values at 298.15 K in the electrochemical
series (provide the reference: see e.g. Atkinsโ€™ Physical Chemistry or CRC Handbook
of Physical Constants). Outline possible sources of errors that might explain any
discrepancies between your value and reference values.
Answer the following post-practical questions:
1) The dominant contribution to the entropy change of the cell reaction is the
reduction of the [Fe(CN6)]3โ€“ ion to [Fe(CN)6]4โ€“. Comment on the possible origin of the
relatively large magnitude and sign of the entropy change that you find in the cell
reaction.
The entropy for the cell was calculated to be -231.5648JK-1.The entropy change in
0
the cell correlates to the negative effect of temperature on ๐ธ๐‘๐‘’๐‘™๐‘™
.
2) Compare the value of the slope obtained from your experiments with that
expected from Nernstโ€™s equation and calculate the percentage error of your result
with respect to the tabulated value
[๐น๐‘’ 3+ ]
The slope of the plot of the change in Ecell with ln([๐น๐‘’ 2+ ]) was found to be
0.0217.However when calculated from the values it is given by,
๐‘…๐‘‡
๐‘›๐น
, the slope was
calculated to be 0.02535. The percentage error in the result was 14.4%
3) Given that the standard entropies of Cu and Zn bulk metals are respectively 33.4
and 41.6 JK-1mol-1 and that those for the Cu2+ and Zn2+ ions in aqueous solution are
-98.7 and -106.5 JK-1mol-1, calculate ๏„S0 for the reaction:
Zn(s) + Cu2+(aq) ๏‚ฎ Zn2+(aq) + Cu(s)
Comment on why the change in entropy is relatively small.
-148.1+132.1=-16 JK-1mol-1
The change in entropy is small for the reaction because the reduction of Cu2+(aq) to
Cu(s) has a positive entropy change, i.e. it is not favored for that part of the reaction
to take place.
PChem Experiment 1
Pre-practical questions:
(1) What is the purpose of the salt-bridge used in this experiment?
The salt bridge allows the flow of charge between cells exclusively in the form of
positively charged ions. It allows the flow of charge without allowing the
chemicals involved in the respective reduction and oxidation reactions to react
with each other.
(2) Write the cell equation (conventional electrochemical specification of the cell) for
this cell reaction.
๐‘ฆ๐‘–๐‘’๐‘™๐‘‘๐‘ 
๐‘๐‘› (๐‘ ) + 2[๐น๐‘’(๐ถ๐‘)6 ]3โˆ’ โ†’
๐‘๐‘›2+ (๐‘Ž๐‘ž) + 2[๐น๐‘’(๐ถ๐‘)6 ]4โˆ’
Name: ___________Louis Gregg_______________________
Student Number: ______10336691_____________________
Date ____________03/10/2011__________________________
Demonstrator ______________________________