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Chemistry 2720
Fall 1995 midterm examination

All questions are weighted equally.

    1. 2% of the maple sap is sugar so we want

      displaymath424

      The mass of sap required is therefore 5kg.

    2. Sap is mostly water. We need to raise the temperature of the water from tex2html_wrap_inline426 to tex2html_wrap_inline428 and then boil it away. Note that there is 4.9kg of water (98% of 5kg) but, guessing that the heat capacity of sugar is similar to that of water, we could reasonably use 5kg as the mass of water to heat.

      eqnarray12

      The total heat which must be provided is therefore

      displaymath430

      This heat comes from burning decane so

      displaymath432

    1. Lavoisier's proposal was essentially that cells are heat engines. The maximum efficiency of a heat engine operating between tex2html_wrap_inline434 and tex2html_wrap_inline428 is

      displaymath438

      The heat to run this engine is provided by burning glucose. The heat of combustion of glucose is just tex2html_wrap_inline440 for the reaction

      displaymath442

      Looking at the data sheet, we see that we have limited information at our disposal. We don't have the heat capacity of glucose so we can't work out the enthalpy of combustion at tex2html_wrap_inline428 , which is what we really need. (The fire would be burning in the hot organelle in this model.) We also only have data gaseous oxygen and carbon dioxide whereas the reactions in a cell would certainly involve the dissolved forms. Our numbers are therefore going to give only a rough approximation, but of course the maximal efficiency calculated above can only give us wildly optimistic estimates anyway. (Obviously, I don't expect you to tell me all this on an exam.)

      eqnarray49

      The efficiency is the work performed divided by the heat input. Therefore

      displaymath446

    2. Isothermal free energy machines are far more efficient than heat engines. The maximum work for an isothermal free energy machine is calculated by computing the change in free energy:

      eqnarray68

      The maximum work is therefore tex2html_wrap_inline448 , or over five times as much as is available from the equivalent heat engine.

  1. The overall process is

    displaymath450

    where G represents a glucose molecule. tex2html_wrap_inline452 for this process is -31.3kJ/mol since the standard free energy of formation of glucose is the same inside as outside the cell. The maximum ratio of glucose in to glucose out is maintained when tex2html_wrap_inline454 . (This means that all of the free energy from the reaction is used to transport glucose.) Therefore

    displaymath456

    assuming that the activity of water is 1 and with the understanding that each concentration term should be divided by 1mol/L to convert it to an activity. Therefore

    displaymath458

    so that

    eqnarray116

    1. The vapour pressure is related to the evaporation process:

      displaymath460

      The equilibrium constant for this process is

      displaymath462

      so the equilibrium constant is the vapour pressure. The standard change in free energy is

      displaymath464

      Therefore

      displaymath466

      (I have cheated slightly and converted from the dimensionless activity to pressure directly.)

    2. There are at least two ways to solve this problem:
      Method 1: At the temperature at which a phase change occurs, tex2html_wrap_inline468 . This implies that tex2html_wrap_inline470 . For this process

      displaymath472

      We have tex2html_wrap_inline474 at 298K and tex2html_wrap_inline440 so

      displaymath478

      If you prefer the Celcius scale, that's about tex2html_wrap_inline480 .

      Method 2: Since the vapour pressure is just an equilibrium constant, we can use the equation which relates equilibrium constants to temperature. At the boiling point, the vapour pressure is 1atm.

      displaymath482

      In our case, let the label tex2html_wrap_inline484 . Calculate tex2html_wrap_inline440 as above and solve for tex2html_wrap_inline488 :

      displaymath490

  2. The formation reaction for steam is

    displaymath492

    Since both enthalpy and free energy are state functions, we imagine converting hydrogen and oxygen at 500K to steam at 500K by the following path:

    1. Cool the hydrogen and oxygen from 500K to 298K. For this step,

      eqnarray239

    2. React the hydrogen and oxygen to form steam at 298K:

      eqnarray281

    3. Heat the steam from 298K to 500K.

      eqnarray306

    For the complete process at 500K,

    eqnarray341


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Up: Back to the old Chemistry 2720 index

Marc Roussel
Sat Oct 12 21:55:20 MDT 1996