Chapter 3: Problem 1
A real gas closely approaches the behaviour of an ideal gas at (a) 15 atmospheres and \(220 \mathrm{~K}\) (b) 1 atm and \(273 \mathrm{~K}\) (c) \(0-5 \mathrm{~atm}\) and \(500 \mathrm{~K}\) (d) 15 atm and \(500 \mathrm{~K}\)
Chapter 3: Problem 1
A real gas closely approaches the behaviour of an ideal gas at (a) 15 atmospheres and \(220 \mathrm{~K}\) (b) 1 atm and \(273 \mathrm{~K}\) (c) \(0-5 \mathrm{~atm}\) and \(500 \mathrm{~K}\) (d) 15 atm and \(500 \mathrm{~K}\)
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Get started for freeAn ideal gas, obeying kinetic theory of gases, can be liquefied: (a) It cannot be liquefied at any \(P\) and \(T\) (b) Its pressure is more than \(P\) at a temperature less than \(T\) (c) Its temperature is more than critical temperature \(T\) (d) Its pressure is more than critical pressure \(P\)
An ideal gas cannot be liquefied because (a) its critical temperature is always above \(0^{\circ} \mathrm{C}\) (b) its molecules are relatively smaller or in size (c) it solidifies before becoming a liquid (d) forces operative between its molecules are negligible
According to the van der Waals correction to get the pressure of ideal gas in observed pressure a definite fraction for correction is (a) subtracted (b) added (c) divided (d) unchanged
The gas that is heated up during Joule-Thomson effect at ordinary temperature is: (a) \(\mathrm{O}_{2}\) (b) \(\mathrm{CO}_{2}\) (c) \(\mathrm{H}_{2}\) (d) \(\mathrm{SO}_{2}\)
Degrees of freedom in a water molecule are (a) 1 (b) 2 (c) 3 (d) 4
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