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Thermodynamics Test - 58

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Thermodynamics Test - 58
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  • Question 1
    1 / -0
    What is the ratio of work done by a ideal monoatomic gas to heat supplied to it in isobaric process.
    Solution

  • Question 2
    1 / -0
    $$p-V$$ diagram of a diatomic gas is a straight line passing through origin. The molar heat capacity of the gas in the process will be:
    Solution

  • Question 3
    1 / -0
    The efficiency of a heat engine if the temperature of source $$227^0C$$ and that of sink is $$27^0C$$ nearly
    Solution
    The efficiency of heat engine will be$$:$$
    $${T_{\sin k}}/{T_{source}}$$
    $$ = \left( {273 + 27} \right)/\left( {273 + 227} \right)$$
    $$ = 300/500$$
    $$ = 0.6$$
    So$$,$$ efficiency will be $$0.6$$
    Hence,
    option $$(C)$$ is correct answer.
  • Question 4
    1 / -0
    The relation between U,P and V for an ideal gas is $$U=2+3PV$$. the gas is 
    Solution
    Given:
    U = 2+ 3PV
    $$\Rightarrow U = 2+ 3 nRT$$
    Differentiating with respect to T,
    $$\Rightarrow \dfrac{dU}{dT} = 0+ 3nR\dfrac{dT}{dT}$$
    $$\Rightarrow C_v = 3nR$$
    For 1 mole of a gas, n=1
    $$\Rightarrow C_v =3R$$
    Since the specific heat at constant volume is 3R for triatomic gas in which atoms are non linear,
    Therefore, correct option is C( polyatomic).
  • Question 5
    1 / -0
    Consider a new system of units in which c (speed of light in vacuum), h(Planck's constant) and G (gravitational constant) are taken as fundamental units. Which of the following would correctly represent mass in this new system?
    Solution
    Consideration anew system of units in which speed of light in vaccum$$=e$$Plank's constant$$=h$$
    Gravitational constant$$=G$$
    Mass in the new system
    $$F=\cfrac{1}{2}mv^2=h\gamma$$
    Now,
    Using the method of dimension we say that,
    Here
    $${e}=LT^{-1}$$
    $$[G]=M^{-1}L^3T^{-2}$$
    $$[h]=M^1L^2T^{-2}$$
    Let, $$mac^xG^0h^z$$
    By substituting the dimension of each quantity in both the sides
    $$M=(LT^{-1})^x(M^{-1}L^3T^{-2})^y(ML^2T^{-1})^z\\M=(M^{y+z}L^{x+3y+2z}T^{x-2y-x})$$
    By equating the power of $$M,L\quad and T$$ in both the sides
    $$-y+z=1\\x+3y+2z=0\\-x-2y-z=0$$
    By solving the above equations
    We get,
    $$x=\cfrac{1}{z},y=-\cfrac{1}{z},z=\cfrac{1}{z}$$
    So, $$[m]=e^{1/2}G^{-1/2}h^{1/2}\\ \quad=\sqrt{\cfrac{hc}{G}}$$
  • Question 6
    1 / -0
    In an adiabatic expansion of as gas, its temperature: 
    Solution
    In an adiabatic expansion of a gas, its temperature decreases.
    From 1st law of thermodynamics,
    $$dU=dQ-dW$$
    For adiabatic process, $$dQ=0$$
    Hence, $$dU=-dW$$
    Gas gas expansion, $$dW>0$$  (positive)
    Therefore, $$dU$$ is less than 0, and thus internal energy  decreases.
    This decrease in internal energy manifest itself as a decrease in temperature T. So, the temperature decreases in an adiabatic expansion of a gas. 
  • Question 7
    1 / -0
    During an adiabatic process, the pressure of a gas is found to be proportional to the cube of its temperature. The ratio of $$\frac { C _ { p } } { C _ { v } }$$ for the gas is
    Solution
    Given :
    Pressure, P$$\alpha T^{3}$$
    Solution:
    In an adiabatic process,
    $$T^{\gamma} P^{1-\gamma}= constant$$ ($$\gamma = \dfrac{C_p}{C_v})$$
    $$\Rightarrow T \alpha \dfrac{1}{P^{\dfrac{(1-\gamma)}{(\gamma)}}}$$
    $$\Rightarrow T \alpha P^\dfrac{(\gamma-1)}{\gamma}$$
    $$\Rightarrow P \alpha T^\dfrac{ \gamma}{(\gamma-1)}$$
    Comparing the two relations, we get
    $$ 3 = \dfrac{\gamma}{(\gamma-1)}$$
    $$\Rightarrow 3(\gamma -1) = \gamma$$
    $$\Rightarrow 3\gamma -3 = \gamma$$
    $$\Rightarrow 2\gamma = 3$$
    Therefore, $$\gamma = \dfrac{3}{2} $$
    Hence, correct option is C.



  • Question 8
    1 / -0
    Which  is correct option for the expansion of an ideal gas under adiabatic cend?
    Solution

  • Question 9
    1 / -0
    When an ideal diatomic gas is heated at constant pressure, the fraction of heat energy supplied which is used in doing work to maintain pressure constant is 
    Solution
    $$\textbf{Step 1 - Heat energy required at constant pressure}$$
    Total energy supplied to raise the temperature
    of a diatomic gas at constant pressure,
    $$Q = nC_{P}\triangle T$$                                          $$....(1)$$
    Where $$C_{P}$$ is heat capacity at constant pressure
    $$n$$ is number of moles
    and $$\triangle T$$ is the temperature difference.

    $$\textbf{Step 2 - Energy required for doing work}$$
    We know
    $$Q = \triangle u + w$$
    $$w = Q - \triangle u$$
    $$w = Q - nC_{V}\triangle T$$                                    $$....(2)$$
    here $$C_{V}$$ is heat capacity at constant volume.
    Put equation $$(1)$$ in $$(2)$$
    $$w = nC_{P}\triangle T - nC_{V}\triangle T$$
    $$w = n\triangle T(C_{P} - C_{V})$$
    $$\Rightarrow w = n\triangle T\ R$$                              
    $$[\because C_{P} - C_{V} = R]$$

    $$\textbf{Step 3 - Fraction of heat energy supplied}$$
    So, fraction of heat energy supplied whish is used in doing work
    $$= \dfrac {w}{Q}$$
    $$= \dfrac {nR\triangle T}{nC_{P}\triangle T}$$
    $$= \dfrac {R}{C_{P}}$$
    $$= \dfrac {R}{\dfrac {7}{5}R}$$               $$\textbf{[for distance ideal gas}$$ $$C_{P} = \dfrac {7}{5} R]$$
    $$= \dfrac {5}{7}$$

    Hence option (A) correct.
  • Question 10
    1 / -0

    A bullet of mass 100g moving with 20 m/s strikes a wooden plank and penetrates upto 20cm . Calculate the resistance offered by wooden plank

    Solution
    Given, 
    Mass of bullet$$=100g=10^{-1}m$$
    Velocity of bullet $$V=20\dfrac{m}{s}$$
    Distance travelled inside wood $$x=20cm=\dfrac{1}{5}m$$
    Now , work done in stopping the bullet =kinetic energy of bullet
    $$F×x=\dfrac{1}{2}mv^2$$
    $$F=\dfrac{1}{2×0.2}×10^{-1}×{20}^2$$
    $$F=10^2$$N
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