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Thermodynamics Test - 49

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Thermodynamics Test - 49
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  • Question 1
    1 / -0
    A heat engine is supplied with 250 kJ/s of heat at a constant fixed temperature of $$227^0C$$; the heat is rejected at $$27^0C$$, the cycle is reversible, then what amount of heat is rejected?
    Solution

    The temperature in kelvin scales are $$T_1=273+27=300K,T_2=273+237=500K$$

    $$T_1$$is temperature of sink And$$T_2$$ is temperature of source hence by efficiency we get

    $$\eta=1-\dfrac{T_1}{T_2}=1-\dfrac{Q_1}{Q_2}$$


    $$Q_1=\dfrac{T_1}{T_2}*Q_2=\dfrac{300}{500}*250=150kW$$
  • Question 2
    1 / -0
    An ideal gas expands according to the law $$pV^2$$= const. The molar heat capacity C is
    Solution
    The correct answer is option(B).
    Molar heat capacity, 
    $$C=C_V+\dfrac R{1-K}=C_V+\dfrac R{1-2}=C_V-R$$
  • Question 3
    1 / -0
    A number of small drops of mercury coalesce adiabatically to form a single drop. The temperature of drop
    Solution
    Hint: For the adiabatic process change in heat is 0.

  • Question 4
    1 / -0
    A gas is compared adiabatically till its temperature is doubled. The ratio of his final volume to its initial volume will be :
    Solution
    Using the relation,
    $$ T_1 V_1^{1- \gamma} = T_2 V_2^{1- \gamma }$$ 

    $$ \dfrac {V_2}{V} = \left( \dfrac {T_1}{T_2} \right)^{ 1 - \gamma} = \left( \dfrac {T_1}{2T_2} \right)^{ 1 - \gamma} $$

    or $$ \dfrac {1}{(2)^{ 1 - \gamma}} > \dfrac {1}{2} $$
  • Question 5
    1 / -0
    When an ideal gas at pressure p, temperature T and volume V is isothermally compressed to V/n, its pressure becomes $$\displaystyle p_i$$. If the gas is compressed adiabatically to $$\displaystyle \frac{V}{n}$$, its pressure becomes $$\displaystyle p_a$$. The ratio $$\displaystyle p_i/p_a$$ is $$\displaystyle \left( \gamma = \frac{C_p}{C_V} \right)$$
    Solution
    For isothermal process,
    $$\displaystyle pV=$$ constant.
    Therefore $$\displaystyle p_iV_i = pV$$
    or $$\displaystyle p_i \frac{V}{n} = pV$$
    or $$\displaystyle p_i =np$$                      .....(i)
    For adiabatic process, $$\displaystyle pV^{\gamma} =$$ constant.
    Therefore
    $$\displaystyle p_a(V_a)^{\gamma} = pV^{\gamma}$$
    or $$\displaystyle p_a \left( \frac{V_a}{n} \right)^{\gamma} = pV^{\gamma}$$
    or $$\displaystyle p_a= n^{\gamma} p$$
    From Eqs. (i) and (ii), we get
    $$\displaystyle \frac{p_i}{p_a} = \frac{n}{n^\gamma} = n^{(1- \gamma)}$$
  • Question 6
    1 / -0
    In an adiabatic process.
    Solution
    In adiabatic process there is no heat transfer i.e $$\Delta Q=0$$
  • Question 7
    1 / -0
    During one cycle of a heat engine $$2000$$ calories of heat is supplied and $$1500$$ calories rejected. The amount of work done equals:
    Solution
    Work done equals the difference of heat supplied to the heat lost.
    $$W = Q_{in} - Q_{out}$$
          $$ = 2000-1500$$
          $$=500\ cal$$
          $$=4.186 \times 500 J$$
          $$=2093\ J$$
  • Question 8
    1 / -0
    A gas is compressed at constant pressure $$ 50 N/m^2$$ from a volume of $$ 0m^3$$ to a volume $$ 4m^3 . $$ Energy $$100 J$$ is then added to the gas by heating. Its internal energy is :
    Solution
    Change in volume $$ \triangle V_2 - V_1 = 4 - 10 = -6 m^3 $$
    A volume decreases, work is done on the gas and so it is negative.
    $$ W = p \triangle V = 50 \times (-6) = -300 J $$
    Additional heat supplied $$ (G = + 100 J ) . $$ So, for the first law of thermodynamics change in external energy is given by 
    $$ \triangle U = Q - W  = 100-(-300) = 400J $$
    Internal energy increases by 400 J.
  • Question 9
    1 / -0
    In the P - V diagram below the dashed curved line is an adiabatic process. For a process that is described by a straight line joining two points $$X$$ and $$Y$$ on the adiabat (solid line in the diagram) heat is : (hint : Consider the variations in temperature from $$X$$ to $$Y$$ along the straight line)

    Solution
    Since from point X to Y ,the gas is compressed and since in adiabatic process no heat is lost so the Temperature at Y is greater than the temperature at X
  • Question 10
    1 / -0
    A heat engine is $$20$$% efficient. If the engine does $$500\ J$$ of work every second, how much heat does the engine exhaust every second?
    Solution
    Efficiency in percentage is defined as:
    $$\eta = \cfrac{\text{Work Done}}{\text{Heat energy supplied}} \times 100$$
    $$20 = \cfrac{500}{E_{in}} \times 100$$
    $$E_{in} = 2500\ J$$

    Heat energy exhausted is the difference of the heat energy supplied and effective work done. Hence, heat exhausted is given by:
    $$H = 2500-500 = 2000\ J$$
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