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An open vessel at 27^(@)C is heated unti...

An open vessel at `27^(@)C` is heated until `3//5` of the air in it is expelled. Assuming that the volume of the vessel remains constant, find the temperature to which the vessel has been heated.

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As the vessel is open, pressure and volume remain constant. Thus, if `n_(1)` moles are present at `T_(1)` and `n_(2)` moles are present at `T_(2)`, we can write `PV=n_(1)RT_(1)` and also `PV=n_(2)RT_(2)`
Hence, `" " n_(1)RT_(1)=n_(2)RT_(2)" or " n_(1)T_(1)=n_(2)T_(2) " or " (n_(1))/(n_(2))=(T_(2))/(T_(1))`
Suppose the no. of moles of air originally present=n
After heating, no of moles of air expelled `=(3)/(5)n`
`:. `No. of moles left after heating `=n-(3)/(5)n=(2)/(5)n`
Thus, `n_(1)=n, T_(1)=300" K ", n_(2)=(2)/(5)n, T_(2)=?` Substituting in eqn. (i), we get
`(n)/((2)/(5)n)=(T_(2))/(300)" or "(5)/(2)=(T_(2))/(300)" or "T_(2)=750" K"`
Alternatively, suppose the volume of the vessel=V, i.e., Volume of air initially at `27^(@)C=V`
Volume of air expelled`=(3)/(5)V" :. "` Volume of air left at `27^(@)C=(2)/(5)V`
However, on heating to `T^(@)K`, it would become=V
As pressure remains constant, (vessel being open), `(V_(1))/(T_(1))=(V_(2))/(T_(2)),i.e., (2//5" V")/(300" K")=(V)/(T_(2))" or " T_(2)=750" K"`
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