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Consider a fuel cell that uses methane ("natural gas") as fuel. The reaction is

CH4+2O2⟶2H2O+CO2

(a) Use the data at the back of this book to determine the values of ΔHand ΔGfor this reaction, for one mole of methane. Assume that the reaction takes place at room temperature and atmospheric pressure.

(b) Assuming ideal performance, how much electrical work can you get out of the cell, for each mole of methane fuel?

(c) How much waste heat is produced, for each mole of methane fuel?

(d) The steps of this reaction are

at-electrode:CH4+2H2O→CO2+8H++8e-at-electrode:2O2+8H++8e-→4H2O

What is the voltage of the cell?

Short Answer

Expert verified

(a) The value in the change of enthalpy is -890.36kJand the value in the change of Gibbs free energy is -817.9kJ.

(b) The electrical work done for each mole of methane fuel is -817.9 kJ.

(c) The amount of waste heat produced for each mole of methane fuel is 72.46 kJ.

(d) The voltage of the cell is 1.061 V.

Step by step solution

01

Explanation

Given:

The transition is

CH412O2,2H2O∣CO2

The temperature is 208k and the pressure is 1 bar.

Formula used:

Write the expression for Gibbs energy-

G=H-TS

Here, G is Gibbs energy, I is the enthalpy, T is the absolute Write the expression for the infinitesimal change in G.

ΔG=ΔH-TΔSm…(1)

Write the expression for the change in enthalpy for the reaction

ΔG=2ΔGH2O+ΔGCO2-ΔGCH4-2ΔGO2……..(3)

02

Calculation

Refer table at the back of the book.

Substitute -393.51kJforΔHCO2,-285.83kJfor ΔHH2O,0for ΔHO2and -74.81kJfor ΔHCH4from the table in expression (2).

Thus, the value in the change of enthalpy is -890.36kJ and the value in the change of Gibbs free energy is -817.9kJ.

03

Step 3. (b) Given information

The reaction is CH4+2O2→2H2O+CO2.

Temperature is 298 K.

Pressure is 1 bar.

Formula used:

Work done, W=∆G

where

G=Gibbs free energy

W=work done

04

Step 4. Calculation

Here, ∆G=-817.9kJ.

So,W=-817.9kJ.

05

Step 5. Conclusion

Hence, the electrical work done for each mole of methane fuel is -817.9 kJ.

06

Step 6. (c) Given information

The reaction is CH4+2O2→2H2O+CO2.

Temperature is 298 K.

Pressure is 1 bar.

As the reaction is occuring at constant pressure.

So,

∆Q=∆Hr-∆Hpwhere∆Q=Energydifference∆Hr=Enthalpychangeforreactants∆Hp=Enthalpychangefortheproducts

07

Step 7. Calculation

As, ∆Hr=890.36kJand ∆Hp=817.9kJ.

So,∆Q=890.36kJ-817.9kJ=72.46kJ

08

Step 8. Conclusion

Hence the amount of waste heat produced for each mole of methane fuel is 72.46 kJ.

09

Step 9. Given information

The reaction is CH4+2O2→2H2O+CO2.

Temperature is 298 K.

Pressure is 1 bar.

Formula for the work done per each electron is

We=W8NAwhereW=workdonepermoleNA=Avogadro'snumber

10

Step 10. Calculation

Here

W=817.9kJNA=6.623×1023

So,

We=817.9kJ86.623×1023=1.061eV

11

Step 11. Conclusion

Hence, the voltage of the cell is 1.061 V.

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Most popular questions from this chapter

Everything in this section so far has ignored the boundary between two phases, as if each molecule were unequivocally part of one phase or the other. In fact, the boundary is a kind of transition zone where molecules are in an environment that differs from both phases. Since the boundary zone is only a few molecules thick, its contribution to the total free energy of a system is very often negligible. One important exception, however, is the first tiny droplets or bubbles or grains that form as a material begins to undergo a phase transformation. The formation of these initial specks of a new phase is called nucleation. In this problem we will consider the nucleation of water droplets in a cloud. The surface forming the boundary between any two given phases generally has a fixed thickness, regardless of its area. The additional Gibbs free energy of this surface is therefore directly proportional to its area; the constant of proportionality is called the surface tension, α

σ≡GboundaryA

ff you have a blob of liquid in equilibrium with its vapor and you wish to stretch it into a shape that has the same volume but more surface area, then u is the minimum work that you must perform, per unit of additional area, at fixed temperature and pressure. For water at 20°C,σ=0.073J/m2

(a) Consider a spherical droplet of water containing N1 molecules, surrounded by N-N1molecules of water vapor. Neglecting surface tension for the moment, write down a formula for the total Gibbs free energy of this system in terms of N,N1, and the chemical potentials of the liquid and vapor. Rewrite N1in terms of V1, the volume per molecule in the liquid, and T, the radius of the droplet.

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The enthalpy and Gibbs free energy, as defined in this section, give special treatment to mechanical (compression-expansion) work, -PdV. Analogous quantities can be defined for other kinds of work, for instance, magnetic work." Consider the situation shown in Figure 5.7, where a long solenoid ( Nturns, total length N) surrounds a magnetic specimen (perhaps a paramagnetic solid). If the magnetic field inside the specimen is B→and its total magnetic moment is M→, then we define an auxilliary field H→(often called simply the magnetic field) by the relation

H→≡1μ0B→-M→V,

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(a) Imagine making an infinitesimal change in the current in the wire, resulting in infinitesimal changes in B, M, and H. Use Faraday's law to show that the work required (from the power supply) to accomplish this change is Wtotal=VHdB. (Neglect the resistance of the wire.)

(b) Rewrite the result of part (a) in terms of Hand M, then subtract off the work that would be required even if the specimen were not present. If we define W, the work done on the system, †to be what's left, show that W=μ0HdM.

(c) What is the thermodynamic identity for this system? (Include magnetic work but not mechanical work or particle flow.)

(d) How would you define analogues of the enthalpy and Gibbs free energy for a magnetic system? (The Helmholtz free energy is defined in the same way as for a mechanical system.) Derive the thermodynamic identities for each of these quantities, and discuss their interpretations.

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The density of ice is 917 kg/m*.

(a) Use the Clausius-Clapeyron relation to explain why the slope of the phase boundary between water and ice is negative.

(b) How much pressure would you have to put on an ice cube to make it melt at -1°C?

(c) ApprOximately how deep under a glacier would you have to be before the weight of the ice above gives the pressure you found in part (b)? (Note that the pressure can be greater at some locations, as where the glacier flows over a protruding rock.)

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(a) Use the first law of thermodynamics to show that, as condensation forms during adiabatic expansion, the temperature of an air mass changes by dT=27TPdP-27LnRdnw

where nw is the number of moles of water vapor present, L is the latent heat of vaporization per mole, and I've assumed f=7/5for air.

(b) Assuming that the air is always saturated during this process, the ratio nw/n is a known function of temperature and pressure. Carefully express dnw/dz in terms of dP/dzanddT/dz, and the vapor pressure PvT. Use the Clausius-Clapeyron relation to eliminate dP/dT.

(c) Combine the results of parts (a) and (b) to obtain a formula relating the temperature gradient, dT/dz, to the pressure gradient, dP/dz. Eliminate Figure 5.18. Cumulus clouds form when rising air expands adiabatically and cools to the dew point (Problem 5.44); the onset of condensation slows the cooling, increasing the tendency of the air to rise further (Problem 5.45). These clouds began to form in late morning, in a sky that was clear only an hour before the photo was taken. By mid-afternoon they had developed into thunderstorms. the latter using the "barometric equation" from Problem 1.16. You should finally obtain dTdz=-27MgR1+PvPLRT1+27PvPLRT2

where " width="9">

(d) Calculate the wet adiabatic lapse rate at atmospheric pressure (I bar) and 25°C, then at atmospheric pressure and 0°C. Explain why the results are different, and discuss their implications. What happens at higher altitudes, where the pressure is lower?

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