Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A muscle can be thought of as a fuel cell, producing work from the metabolism of glucose:

C6H12O6+6O26CO2+6H2O

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

(b) What is maximum amount of work that a muscle can perform , for each mole of glucose consumed, assuming ideal operation?

(c) Still assuming ideal operation, how much heat is absorbed or expelled by the chemicals during the metabolism of a mole of glucose?

(d) Use the concept of entropy to explain why the heat flows in the direction it does?

(e) How would your answers to parts (a) and (b) change, if the operation of the muscle is not ideal?

Short Answer

Expert verified

(a) The value of ΔHis -2803.04kJand the value of ΔGis -2878.94kJ.

(b) The maximum amount of workdone is 2878.94 KJ.

(c) The amount of heat absorbed is 75.9 KJ.

(d) Here, the heat is positive and entropy is positive. So, the heat flows into the system.

(e) Here less amount of energy will leave the system, but Gibbs free energy and enthalpy will be same.

Step by step solution

01

Explanation

The chemical reaction for the fuel cell of the muscle is

C6H12O6+6O26CO2+6H2O

Formula used:

Write the expression for the enthalpy change for the reaction.

ΔH=6HCo2+6HH2O-HC6H12O6-6HO2(1)

Here, HCO2is the enthalpy for CO2,HH2Ois the enthalpy of H2O,HC4H2O4is the enthalpy for C6H12O6and Ho2is the enthalpy of O2.

Write the expression for the Gibbs energy change for the reaction.

ΔG=6GCO2+6GH2O-GCbH12O4-6GO2(2)
02

Calculation

Calculation:

Refer table at the back of the book.

Substitute-285.83kJfor HCO4,-393.51kJfor HH2O,0for HCnH2O6and -1273kJfor Ho2in expression (1).

ΔH=-6(285.83kJ+393.51kJ)-6(0)+1273kJ=-2803.04kJ

Substitute-237.13kJfor GCO2,-394.36kJfor GH2O,0for GC6H2O3and -910kJfor GO2in expression (2).

ΔG=-6(237.13kJ+394.36kJ)-6(0)+910kJ=-2878.94kJ

Thus, the value of ΔH is -2803.04kJ and the value of ΔG is -2878.94kJ.

03

Step 3. (b) GIven information

The chemical reaction for the fuel cell of the muscle is

C6H12O6+6O2→6CO2+6H2O.

Workdone for ideal operation,

W=GwhereW=workdoneG=Gibbsenergy

04

Step 4. Calculation

As, G=2878.94KJ.

So,W=2878.94KJ

05

Step 5. Conclusion

The maximum amount of workdone is 2878.94 KJ.

06

Step 5. Given information

The chemical reaction for the fuel cell of the muscle is

C6H12O6+6O2→6CO2+6H2O.

The enthalpy is less than the amount of the work extracted.

The expression for the heat absorbed.

Q=W-∆H

where

Q=heatabsorbed.

07

Step 7. Calculation

Here

W=2878.94KJH=2803.04KJ

So,Q=2878.94KJ-2803.04KJ=75.9KJ

08

Step 8. Conclusion

The amount of heat absorbed is 75.9 KJ.

09

Step 9. Given information

The chemical reaction for the furl cell of the muscle is

C6H12O6+6O2→6CO2+6H2O.

The expression for the entropy change for the reaction.

S=6SCO2+6SH2O-SC6H12O6-6SO2·······(3)whereSCO2=EntropyforCO2SH2O=EntropyofH2OSC6H12O6=EntropyofC6H12O6SO2=EntropyofO2

Entropy in terms of heat absorbed

S=QT········(4)whereQ=heatabsorbedT=absolutetemperature

10

Step 10. Calculation

From the table

SCO2=69.91J·K-1SH2O=213.74J·K-1SC6H12O6=205.14J·K-1SO2=212J·K-1

So,

S=669.91+213.74=6205.14-212J·K-1=259.06J·K-1

Hence,

Q=259.06J·K-1298K=77.2KJ

11

Step 11. Conclusion

Thus, the heat is positive and entropy is also positive. So, the heat flows into the system.

12

Step 12. Given information

The chemical reaction for the fuel cell of the muscle is

C6H12O6+6O2→6CO2+6H2O.

In the ideal reaction, the work equals the change in the Gibbs energy. But when the reaction is not ideal the amount of work is less than the Gibbs energy. Here, as the change of entropy is same, therefore less heat flow enters the system and less energy leaves the system. But, the Gibbs free energy and enthalpy are same whether or not the operation is ideal or not.

13

Step 13. Conclusion

Thus, less amount of energy will leave the system, but Gibbs free energy and enthalpy will be same.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Calculate the Helmholtz free energy of a van der Waals fluid, up to an undetermined function of temperature as in equation5.56. Using reduced variables, carefully plot the Helmholtz free energy (in units of NkTc) as a function of volume for T/Tc=0.8Identify the two points on the graph corresponding to the liquid and gas at the vapor pressure. (If you haven't worked the preceding problem, just read the appropriate values off Figure5.23.) Then prove that the Helmholtz free energy of a combination of these two states (part liquid, part gas) can be represented by a straight line connecting these two points on the graph. Explain why the combination is more stable, at a given volume, than the homogeneous state represented by the original curve, and describe how you could have determined the two transition volumes directly from the graph of F.

Write down the equilibrium condition for each of the following reactions:

(a)2HH2(b)2CO+O22CO2(c)CH4+2O22H2O+CO2(d)H2SO42H++SO42-(e)2p+2nHe4

Use the data at the back of this book to verify the values of ΔH and ΔGquoted above for the lead-acid reaction 5.13.

At temp 298K and pressure 1 bar.

Suppose you need a tank of oxygen that is 95% pure. Describe a process by which you could obtain such a gas, starting with air.

The formula for CP-CV derived in the previous problem can also be derived starting with the definitions of these quantities in terms of U and H. Do so. Most of the derivation is very similar, but at one point you need to use the relation P=-(F/V)T.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free