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    The Deviation Of Real Gas From Ideal Gas Behavior - Practice Questions & MCQ

    Edited By admin | Updated on Sep 18, 2023 18:35 AM | #JEE Main

    Quick Facts

    • Behaviour of Real Gases: Deviation from Ideal Gas Behaviour is considered one of the most asked concept.

    • 62 Questions around this concept.

    Solve by difficulty

    The term that corrects for the attractive forces present in a real gas in the van der Wals equation is -

    Positive deviation from ideal behaviors takes place because of:

    A gas will approach ideal behaviour of -

    In Van der Waals's equation of state for a non-ideal gas, the term that accounts for intermolecular forces is -

    The temperature at which a real gas obeys the ideal gas laws over a wide range of pressure is -

    At a given temperature T , gases $\mathrm{Ne}, \mathrm{Ar}, \mathrm{Xe}$ and kr are found to deviate from ideal gas behaviour

    $
    \mathrm{P}=\frac{\mathrm{RT}}{\mathrm{~V}-\mathrm{b}} \text { al } \mathrm{T}
    $


    This equation of state is given as, $\mathrm{P}=\frac{\mathrm{R}}{\mathrm{V}-\mathrm{b}}$ al T . Which gas will exhibit steepest increase in the plot of ?

    The force of attraction among molecules should be neglected at

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    Which of the following is known as Van der waal constant?

    Which of the statement is correct

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    Which curve in Fig. 5.2 represents the curve of ideal gas?

     

    Concepts Covered - 0

    Behaviour of Real Gases: Deviation from Ideal Gas Behaviour

    Ideal Gas: 
    These gases obey gas laws under all the conditions of temperature and pressure,

    • No gas is ideal in reality (hypothetical). 

    • No force of attraction is present between molecules in them. 

    • Volume of molecules is negligible to the total volume of the gas (container).

    Real Gas:
    These gases obey gas laws only at high temperature and low pressure. 

    • All the gases are real. 

    • Here the force of attraction between molecules cannot be neglected at high pressure and low temperature.

    • Here volume occupied by gas molecule is not negligible specially at high pressure and low temperature.

    Behaviour of Real Gases: Deviation from Ideal Gas Behaviour and Compressibility factor Z



    The extent of deviation of a real gas from ideal gas behaviour is expressed in terms of compressibility factor Z. It is an empirical correction for the non-ideal behaviour of real gases which allows the simple form of the combined gas law to be retained It is given as:
    \mathrm{Z=\frac{P V}{n R T}}
    When Z = 1 (ideal gas behaviour)

    When Z < 1 (negative deviations)

    When Z > 1 (positive deviations)

    When Z < 1 gas is more compressible 

    When Z > 1 gas is less compressible

    • For He and H2 , Z > 1 as PV>RT [as a/V2 = 0 ] that is, positive deviations.
    • At very Low Pressure: PV RT (as a/V2  and b are neglected) that is, Z 1 so nearly ideal gas behaviour. 
    • At Low Pressure: PV<RT that is, Z < 1 so negative deviation 
    • At Moderate Pressure : PV = RT i.e, Z = 1 so ideal gas behaviour 
    • At High Pressure: PV > RT (as b can not be neglected). that is, Z > I so positive deviation.
    • An increase in temperature shows a decrease in deviation from ideal gas behaviour.

    Plot of pV vs p for real gas and ideal gas

    Plot of pressure vs volume for real gas and ideal gas

    Van der Waal’s Equation
    Van der waal's equation is a modification of the ideal gas equation that takes into account the non-ideal behaviour of real gases Van der Waal 's equation modified kinetic theory of gases by considering these two points of kinetic theory of gases not to be fully correct or are not followed by real gases.
    For an ideal gas the force of attraction between gaseous molecules is negligible and the volume of gaseous molecules is negligible to the total volume of the gas. These two assumptiions are not followed by real gases.


    He made following two corrections :

    • Volume Correction
      According to him, at high pressure the volume of the gas becomes lower so volume of molecules can not be ignored Hence the actual space available inside the vessel for the movement of gas molecules is not the real volume of the gas, actually it is given as:
      Vreal gas = V - b
      Here V is the volume of the container while b is the volume occupied by gas molecules and it is called co-volume or excluded volume. 
      The excluded volume for 'n' molecules of a gas = 4nVm or (4 x 4/3𝜋r3)
      Here Vm = Volume of one molecule (4/3𝜋r3
      Thus, the ideal gas equation can be written as:
      P(V-nb) = nRT

    • Pressure Correction
      According to him, the gaseous molecules are closer so attraction forces cannot be ignored hence, pressure of the real gas is given as: 
      Pressure of the Real gas = pressure developed due to collisions (P) + pressure loss due to attraction (p')
      \mathrm{P_{real\: gas}=P+p^{\prime}}
      Here p' is pressure loss due to force of attraction between molecules or inward pull
      \\\begin{array}{l}{\text{As}:p^{\prime} \propto n^{2},\left[n^{2} \text { is the number of molecules attracting or attracted }\right]}\\{p^{\prime} \propto n^{2} \propto d^{2} \propto \frac{1}{V^{2}}}\end{array}
      \mathrm{Thus,\: p^{\prime}=\frac{a}{V^{2}}=\frac{a n^{2}}{V^{2}}} (for n moles of gas)
      Here 'a' is Van der Waal's force of attraction constant, d is density and V is volume.
      Hence
      \begin{array}{l}{P_{real\:gas}=P+a / V^{2}}\end{array}

    \mathrm{P_{\textup{Real gas }}= {P+\frac{n^{2} a}{V^{2}} \ldots \ldots(2)}} (for n moles of gas)

    • Now ideal gas equation can be written after correction of pressure and volume for n moles
      \mathrm{\left(P+\frac{n^{2} a}{V^{2}}\right) \cdot(V-n b)=n R T}

    • Units of a and b
      \begin{aligned} \mathrm{a}=& \text { lit}^{2} \, \mathrm{mol}^{-2}\, \mathrm{atm} \\ & \text { or } \mathrm{cm}^{4}\, \mathrm{mol}^{-2} \, \mathrm{dyne} \\ & \text { or } \mathrm{m}^{4} \, \mathrm{mol}^{-2} \text {Newton } \\ \mathrm{b}=& \text { lit/mol } \\ & \text { or } \mathrm{cm}^{3} / \mathrm{mol} \\ \text {or} & \: \mathrm{m}^{3} / \mathrm{mol} \end{aligned}
      The values of 'a' and 'b' are 0.1 to 0.01 and 0.01 to 0.001 respectively.

    Variation of compressibility factor for some gases

    Value of Compressibility Factor at High P and Low P

    Explanations for Real Gas Behaviour

    • At very low pressure for one mole of a gas, the value of 'a' and 'b' can be ignored so Van der Waal's equation becomes equal to ideal gas.
      PV=RT 
    • At low pressure, the value of 'nb' or 'b' can be ignored so Van der Waal's equation becomes

      \begin{array}{l}{\left[P+a / V^{2}\right][V]=R T} \\\\ {P V+\frac{a}{V}=R T} \\\\ {P V=R T-\frac{a}{V}}\end{array}

      Hence PV < RT
      so,
      \begin{array}{l}{Z=\frac{PV}{RT}} \\\\ {Z<1}\end{array}

    • At moderate pressures, neither the value of 'a' nor 'b' can be neglected and we have to consider both the value of 'a' as well as 'b' for the calculation of Z.

    • At high pressure, the value of 'a' can be ignored so Van der Waal's equation can be written as

      \begin{array}{l}{P(V-b)=R T} \\\\ {P V-P b=R T} \\\\ {P V=R T+P b} \\\\ {Z=\frac{P V}{R T}} \\\\ {S o, Z>1}\end{array}

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