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Thermodynamics Test - 34

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Thermodynamics Test - 34
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  • Question 1
    1 / -0
    Two samples $$A$$ and $$B$$ of a gas initially at the same pressure and temperature are compressed from volume $$V$$ to $$\displaystyle\frac{V}{2}$$ ($$A$$ isothermally and $$B$$ adiabatically). The final pressure of $$A$$ is
    Solution
    For isothermal process, $$PV =$$ constant
    $$P_1V_1 = P_2V_2$$
    $$\implies P_2 = 2P_1$$

    For adiabatic process, $$ P {V}^{\gamma} $$ = constant
    $$P_1V_1^{\gamma} = P_2V_2^{\gamma}$$
    $$\implies P_2 = P_1 (\dfrac{V_1}{V_2})^{\gamma}$$
    $$ \implies P_2 = P_1 2^{\gamma}$$

    Since, $$ \gamma $$ is always greater than 1, For the same change in volume, there will be a greater change in pressure for adiabatic process than that for isothemral process.
  • Question 2
    1 / -0
    Four curves $$A$$, $$B$$, $$C$$ and $$D$$ are drawn in figure for a given amount of gas. The curves which represent adiabatic and isothermal changes are.

    Solution
    The PV graph is always a rectangular hyperbola with its asymptotes as the positive x and y axes.
    However, $$the \ slope\ of\ the\ adiabatic\ curve\ is\ \gamma \ times\ the\ slope\ for\ an\ isothermal\ curve.$$

    Thus, A curve is for adiabatic and B for isothermal.
  • Question 3
    1 / -0

    Directions For Questions

    The temperature of $$3\:kg$$ of nitrogen is raised from $$10^\circ C$$ to $$100^\circ C$$ at constant pressure.
    For nitrogen $$C_p=1400\:J/kgK$$ and $$C_v=740\:J/kgK$$

    ...view full instructions

    Compute the change in internal energy (in joules)
    Solution
    The change in internal energy is given by,
    U = $$ m {C}_{v} \Delta T $$(m is used because $$C_p$$ and $$C_v$$ are given per kg)
    U = 3 $$ \times 740 \times (100 - 10) $$
    $$U = 199800 J$$
  • Question 4
    1 / -0

    Directions For Questions

    The temperature of $$3\ moles$$ of nitrogen is raised from $$10^\circ C$$ to $$100^\circ C$$ at constant volume.
    For nitrogen $$C_p=1400\:J/kgK$$ and $$C_v=740\:J/kgK$$

    ...view full instructions

    Compute the work done (in joules)
    Solution
    For the processes taking place at constant volume, the work done is always zero. Hence B is correct answer.
  • Question 5
    1 / -0
    A container of volume $$1\:m^3$$ is divided into two equal compartments by a partition. One of these compartments contains an ideal gas at $$300\:K$$. The other compartment is vacuum. The whole system is thermally isolated from its surroundings. The partition is removed and the gas expands to occupy the whole volume of the container. Its temperature now would be :
    Solution

  • Question 6
    1 / -0
    An ideal gas $$\displaystyle\left(\frac{C_p}{C_v}=\gamma\right)$$ is taken through a process in which the pressure and the volume vary as $$P=aV^b$$. The value of b for specific heat capacity as zero is
    Solution
    Given that $$P=aV^b$$
    or $$PV^{-b}=a$$
    Comparing with $$PV^r=constant$$, we have
    $$r=-b$$
    We know that molar specific heat $$\displaystyle C=C_v-\dfrac{R}{r-1}$$

    $$\displaystyle\therefore 0=\dfrac{R}{\gamma-1}-\dfrac{R}{-b-1}$$

    or $$b=-\gamma$$
  • Question 7
    1 / -0
    A thermally insulated container is divided into two parts by a screen. In one part the pressure and temperature are $$P$$ and $$T$$ for an ideal gas filled. In the second part it is vacuum. If now a small hole is created in the screen, then the temperature of the gas will
    Solution
    According to the ideal gas law, PV = nRT,  
    Since the will be a change in volume of gas occurs slowly i.e. process occurs isothermally.
    (To compensate for the change in volume, there will be a corresponding change in the pressure of the gas, therefore the temperature will tend to remain constant.)
  • Question 8
    1 / -0
    In an adiabatic process pressure is increased by $$\displaystyle\frac{2}{3}\%$$ if $$\displaystyle\frac{C_p}{C_v}=\frac{3}{2}$$. Then the volume decrease by about
    Solution
    In an adiabatic process, $$PV^{\gamma}=constant$$
    $$\gamma=\dfrac{C_P}{C_V}=\dfrac{3}{2}$$
    Thus $$P_0V_0^{\gamma}=P_0(1+\dfrac{2/3}{100})V^{\gamma}$$
    $$\implies V=\dfrac{V_0}{(1+\dfrac{2/3}{100})^{1/ \gamma}}$$
    $$=V_0(1+\dfrac{2/3}{100})^{-2/3}$$
    $$\approx V_0(1-\dfrac{4/9}{100})$$
    Thus, volume decreases by $$\dfrac{4}{9}$$%
  • Question 9
    1 / -0
    For process 1, $$\Delta U$$ is positive, for process 2, $$\Delta U$$ is zero and for process 3, $$\Delta U$$ is negative. Find the parameters indicating $$x$$ and $$y$$ axes.

    Solution
    $$\Delta U=0  \Rightarrow \Delta T=0\Rightarrow$$ isothermal process
    Similarly $$\Delta T >0$$ for 1 and $$<0$$ for 3.
    Thus starting from same pressure(P) and volume(V) and reaching same final volume the values of pressure will be $$P_1>P_2>P_3$$
    Clearly x, y axes are thus volume and pressure axes respectively. 
  • Question 10
    1 / -0
    On an isothermal process, there are two points $$A$$ and $$B$$ at which pressures and volumes are $$(2P_o,\:V_o)$$ and $$(P_o,\:2V_o)$$ respectively. If $$A$$ and $$B$$ are connected by a straight line, find the pressure at a POINT on this straight line at which temperature is maximum
    Solution
    Using symmetry, the temperature will be maximum at a point where the pressure and the volume attain the same value.
    Therefore, on a straight line, joining the 2 points A and B as given in the question, the temperature will be maximum at their midpoint. 
    Hence, the pressure will be $$ \dfrac{3 {P}_{o}}{2} $$ and the volume will be $$ \dfrac{3 {V}_{o}}{2} $$
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