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Thermodynamics Test - 46

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Thermodynamics Test - 46
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  • Question 1
    1 / -0
    In above shown figure of refrigeration system. Which of the following statement explains why work is an input into this system?

    Solution
    In a thermodynamic system, heat naturally flows from hotter body to a colder body. The given figure shows a refrigerator energy flow diagram. The heat flow is opposite to the direction of conventional heat flow and hence external work is required for the given heat flow diagram.
  • Question 2
    1 / -0
    In a thermodynamic processes during each cycle , a heat engine absorbs 400 J of heat from a higher- temperature source and release 300 J of heat to the low-temperature sink. Calculate the efficiency of heat engine?
    Solution
    The efficiency of heat engine, $$\eta=\dfrac{W}{Q_1}=\dfrac{Q_1-Q_2}{Q_1}=\dfrac{400-300}{400}=1/4$$ 
  • Question 3
    1 / -0
    A heat engine takes in heat at 750 degrees Celsius and expels heat at 250 degrees Celsius. What is this engine's theoretically ideal (Carnot) efficiency?
    Solution
    Temperature of source     $$T_H = 750^oC = 750+273 = 1023$$  K
    Temperature of sink     $$T_L = 250^oC = 250+273 = 523$$  K

    Efficiency of engine        $$\eta = 1-\dfrac{T_L}{T_H} = 1  -\dfrac{523}{1023}  =0.49$$
    Thus the engine is  $$49$$% efficient.
  • Question 4
    1 / -0
    Find out the efficiency of the heat engine if it produces $$100 J$$ of heat, does $$30 J$$ of work, and emits $$70 J$$ into a cold reservoir.
    Solution
    Efficiency of a heat engine is given by ,
               $$\eta=\dfrac{W}{Q_{1}}$$ 
    where $$W=$$ net work done /cycle  and  $$Q_{1}=$$total heat absorbed / cycle
                given - $$W=30J$$  , $$Q_{1}=100J$$
       therefore  $$\eta=\dfrac{30}{100}\times100=30$$%
  • Question 5
    1 / -0
    A heat engine produces 100 J of heat, does 30 J of work, and emits 70 J into a cold reservoir. What is the efficiency of the heat engine? 
    Solution
    The efficiency of heat engine is $$\eta=\dfrac{W}{Q_{in}}$$  
    Here work done , $$W=30 J$$ and heat produced $$Q_{in}=100 J$$
    Thus, % of efficiency, $$\eta=\dfrac{30}{100}\times 100=30$$ %
  • Question 6
    1 / -0
    The idealized P-V diagram above shows a complete cycle through compression and expansion of a gas. The questions below relate to the processes within the cycle.
    Which letter shows work done?

    Solution
    Here the  work done will be the area under the pressure-volume curve. The work done under the part A will be positive work, but the negative work done under the part C  must be subtracted. Thus the leaving work as E as shown in diagram. Thus, option E will be correct. 
  • Question 7
    1 / -0
    During a cyclic thermodynamic process, a gas absorbs 45 J of heat.
    Which table correctly describes the change in internal energy in the gas and work done by the gas during this cycle?
    Solution
    As heat is absorbed by the gas,    $$\implies$$ $$Q = + 45$$ J
    Change in internal energy of the gas during one cycle is zero  i.e   $$\Delta U =0$$ J
    From 1st law of thermodynamics :          $$Q = \Delta U + W$$
    $$\therefore$$   $$45 = 0+ W$$                     $$\implies W = +45$$ J
    Thus the work done by the gas is  $$45$$ J.
  • Question 8
    1 / -0
    The thermal capacity of $$10$$gm of the substance is $$8$$ calories. Then its specific heat is.
    Solution
    thermal capacity=specific heat *mass, mass=density*volume.
    specific heat =$$\dfrac{Thermal.capacity}{mass}=\dfrac{8}{10}=0.8$$
  • Question 9
    1 / -0
    For a particular heat engine, 3,000 J of energy goes in at 700 K and 2000 J comes out at 200 K. The rest of the energy is used work.
    What is the actual efficiency of this engine?
    Solution
    Amount of heat goes in the engine        $$Q_H = 3000$$ J
    Amount of heat rejected by the engine      $$Q_R = 2000$$ J
    Thus work done by the engine      $$W = Q_H - Q_R =3000 - 2000 = 1000$$ J

    Actual efficiency of heat engine       $$\eta = \dfrac{W}{Q_H} = \dfrac{1000}{3000} = 0.33$$
  • Question 10
    1 / -0
    A liquid is being converted into vapours at its boiling point the specific heat of the liquid at this temperature will be.
    Solution
    The boiling point of a liquid is defined as the temperature at which the vapour pressure of the liquid becomes equal to the atmospheric pressure. Therefore, at boiling point, specific heat of a liquid is equal to the specific heat of vaporization of that liquid.
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