Conceptual Questions (5 points each)


Questions 1 -- 6 refer to the following situation:


Mystery substance X has the following thermodynamic data:


tabular30


  1. How much heat is required to heat 1 kg of liquid X from 10 tex2html_wrap_inline276 C to 210 tex2html_wrap_inline276 C?

    (c) 100 kcal

    To heat liquid X through tex2html_wrap_inline280 C requires

    displaymath282

  2. How much heat is required to boil 1 kg of liquid X at 210 tex2html_wrap_inline276 C?

    (d) 150 kcal

    To boil liquid X at 210 tex2html_wrap_inline276 C requires

    displaymath288

    Note that tex2html_wrap_inline290 , the heat of vaporization, applies to boiling the liquid; not tex2html_wrap_inline292 , the heat of fusion, which applies to the melting/freezing transition.

  3. What is the fractional change in its volume, when liquid X decreases in temperature by 10 tex2html_wrap_inline276 C?

    (d) Liquid X's volume decreases by 4%.

    The fractional change in volume, for tex2html_wrap_inline296 C, is

    displaymath298

    for a decrease of 4%.

  4. A sample of liquid X at 80 tex2html_wrap_inline276 C sits in a 0 tex2html_wrap_inline276 C room, and cools by radiation only. It loses energy at the rate 1 W. If the room temperature were increased to 40 tex2html_wrap_inline276 C, at what rate would the 80 tex2html_wrap_inline276 C sample of liquid X now lose energy?

    (c) 0.6 W

    The sample loses radiative energy because it emits more energy than it absorbs. Specifically, it loses energy at the rate

    displaymath308

    where all temperatures are expressed in Kelvin. When the room temperature is increased to tex2html_wrap_inline310 C, this rate changes because tex2html_wrap_inline312 is altered by a factor

    displaymath314

    Since the old rate of energy loss, tex2html_wrap_inline316 , is given as 1 W, the rate in the warmer room must be 0.6 W.


    Questions 5 and 6 pertain to the following specific process undergone by substance X:


    1 kg of substance X is heated from an initial temperature of -10 tex2html_wrap_inline276 C to a final state which is a mixture of 0.3 kg of liquid X and 0.70 kg of gas X.


  5. Which one of the following is an accurate qualitative depiction of the sample's evolution in pressure and temperature?

    tex2html_wrap438 tex2html_wrap440

  6. Which one of the following is an accurate qualitative depiction of the sample's temperature variation as heat is added?

    tex2html_wrap442 tex2html_wrap444

    Questions 7 through 12 pertain to the situation described below:

    An ideal monatomic gas originally in state A at temperature 27 tex2html_wrap_inline276 C can be taken to state B at temperature tex2html_wrap_inline332 via any of the thermodynamic processes shown.

    tex2html_wrap446
    For these questions you may choose to use the ideal gas constants tex2html_wrap_inline334 , though they are not strictly necessary.

  7. Which of the following is an accurate ordering of the amount of work done (W) by the gas in each of these processes?

    (a) tex2html_wrap_inline338

    Work done by the gas is given by the area under the PV curve. By inspection (for example, counting up full boxes under the curves), this is greatest for I, then smaller for II, then III, then IV.

  8. How much work is done by the gas in process I? (Note the conversion factor 1 atm l = 100 J.)

    (b) 600 J

    Process I occurs at constant pressure, so the work done by the gas is just

    displaymath342

    which, given the conversion factor, is 600 J.

  9. What is the temperature of the gas in state B?

    (d) 327 tex2html_wrap_inline276 C

    This can be found from the ideal gas law, for constant n, where all temperatures must be expressed in Kelvin:

    displaymath348

  10. In process III, the gas expands from state A to state C isothermally, doing 480 J of work. What is the change in entropy ( tex2html_wrap_inline350 ) for the gas during the isothermal process AC?

    (b) 1.6 J/K

    Since the ideal gas expands isothermally, tex2html_wrap_inline352 and Q= W = 480 J. tex2html_wrap_inline350 is just defined as Q/T, where T is the temperature of the constant temperature process, expressed in Kelvin. This is given as tex2html_wrap_inline362 , so

    displaymath364


    Questions 11 and 12 both refer to process IV, where the gas expands from state A to state D adiabatically, with tex2html_wrap_inline366 C.


  11. What is the change in internal energy of the gas during the adiabatic process AD?

    (a) -225 J

    The change in internal energy, for this ideal monatomic gas, is

    displaymath368

    Here tex2html_wrap_inline370 K. But 150 K is tex2html_wrap_inline372 , so using the ideal gas law we find

    displaymath374

    which gives -225 J using the 1 atm l = 100 J conversion factor.

  12. How much work does the gas do in process IV (for the entire process, from A to D to B)?

    (b) 225 J

    Since process AD is adiabatic, tex2html_wrap_inline378 , telling us the gas does W = 225 J of work from A to D, using our answer to 11. Since process DB is isochoric (constant volume), the gas does no further work from D to B. Thus the gas does a total of 225 J of work in process IV.

    Questions 13 and 14 pertain to the following situation:


    A heat engine operates between a hot reservoir at 1500 K and a cold reservoir at 500 K. tex2html_wrap_inline382 J of heat is removed from the hot reservoir and tex2html_wrap_inline384 J of work is performed.

  13. What is the actual efficiency of this engine?

    (a) 0.15

    The engine has efficiency

    displaymath386

  14. What is the ideal (Carnot) efficiency of this engine?

    (d) 0.67

    The Carnot efficiency of the engine is

    displaymath388

Quantitative Problems (Point Value as Marked)


  1. (30 points)

    A 350 g copper ingot at tex2html_wrap_inline390 C is placed in a calorimeter with 420 g of water at tex2html_wrap_inline392 C. Specific heats for copper, water, and ice are

    tabular167

    while the heat of fusion for water is tex2html_wrap_inline400 .

    1. How much heat would be required to raise the temperature of the copper ingot to tex2html_wrap_inline402 C?
    2. What is the final state of the system? Give both the final temperature, and the masses of water and/or ice present.



    tex2html_wrap448

    tex2html_wrap450

    1. For such heating, the copper must gain

      displaymath412

    2. We use our answer from (a), stating that the copper must gain tex2html_wrap_inline414 to raise its temperature to tex2html_wrap_inline402 C, to help us assess what the final temperature must be. For in this final state, the heat gained by the copper must equal the heat lost by the water.

      First, were the water to cool to tex2html_wrap_inline402 C, it would give up

      displaymath420

      This is not enough to heat the copper to the same temperature, tex2html_wrap_inline402 C, so the water must continue to give up heat.

      Next, were the water to fully freeze at tex2html_wrap_inline402 C, it would give up an additional

      displaymath426

      Together with the heat lost by the water in cooling, this is more than enough to heat the copper to the same final temperature, tex2html_wrap_inline402 C. Thus we know that the final temperature must be tex2html_wrap_inline402 C, with only a portion of the water frozen to ice so that, in reaching the final state, tex2html_wrap_inline432 .

      Setting up this equality,

      eqnarray198

      using our partial results above. Thus

      displaymath434

      and

      displaymath436

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Katherine Benson
Tue Dec 11 14:53:07 EST 2001