- Isotactic
- Saturation
- Inversion
- Throttling
Answer: Option 3 The joule Thomson coefficient is given as $${\mu _i} = {\left( {\frac{{\partial T}}{{\partial P}}} \right)_H},$$ And since for an ideal gas enthalpy is strictly only function...
1 Answers 1 viewsAnswer: Option 1 Above the inversion temperature joule-thomson coefficient $${\left( {\frac{{\partial T}}{{\partial P}}} \right)_H} = - ve$$ So, by throttling (decreasing the pressure) the temperature increases and hence heating. Below the inversion...
1 Answers 1 viewsAnswer: Option 4 When a gas is subjected to adiabatic expansion like throttling any real fluid will lose some of its internal energy (mainly pressure energy if the flow is...
1 Answers 2 viewsAnswer: Option 1 Let'
1 Answers 1 viewsAnswer: Option 1 Above the inversion temperature joul thomson coefficient $$\left( \mu \right) = {\left( {\frac{{\partial T}}{{\partial P}}} \right)_H}{\text{ is }} - {\text{ve}}$$ So, on decreasing the pressure (throttling) the temperature...
1 Answers 1 viewsAnswer: Option 4 Since all the gases except $${H_2}$$ $$He$$ etc, have maximum inversion point greater than atmospheric (room) temperature cooling can take place by throttling if the initial conditions...
1 Answers 1 viewsAnswer: Option 3 For cooling to take place by throttling the Joule-Thomson coefficient must be negative. $${\left( {\frac{{\partial T}}{{\partial P}}} \right)_H} = - VE.$$
1 Answers 1 viewsAnswer: Option 2 Let'
1 Answers 1 viewsAnswer: Option 1 Let'
1 Answers 4 views