At #100^@ "C"# and #"1.00 atm"#, the molar volume of water vapor is #"30.6 L/mol"# and the enthalpy of vaporization is #"40.66 kJ/mol"#. What is the change in internal energy at this temperature for #"1 mol"# of water? (#rho("H"_2"O"(l)) ~~ "996 g/L"#)
You should have the following equation available for a constant pressure process:
You were also given the molar volume of the water vapor, so you can now calculate the change in volume:
which makes sense because the volume of 1 mol of gas is much larger than the volume of 1 mol of the corresponding liquid. So, the change in volume is negative, i.e. the water was greatly compressed during condensation.
Therefore:
and due to the number of sig figs, you'd get the same answer even with the assumption of ignoring the molar volume of liquid water.
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To find the change in internal energy (( \Delta U )) for 1 mole of water at 100°C and 1.00 atm pressure, you can use the equation:
[ \Delta U = \Delta H - P \Delta V ]
Where:
- ( \Delta H ) = enthalpy of vaporization = 40.66 kJ/mol
- ( P ) = pressure = 1.00 atm
- ( \Delta V ) = change in volume = molar volume of water vapor - molar volume of liquid water
Given:
- Molar volume of water vapor = 30.6 L/mol
- Density of water (( \rho )) at 100°C is approximately 996 g/L
First, calculate the molar volume of liquid water using its density:
[ \text{Density of water} = \frac{\text{mass}}{\text{volume}} ] [ \Rightarrow \text{Volume of 1 mole of liquid water} = \frac{\text{mass of 1 mole}}{\text{density of water}} ] [ \Rightarrow \text{Volume of 1 mole of liquid water} = \frac{18 , \text{g/mol}}{996 , \text{g/L}} ]
Now, calculate the change in volume:
[ \Delta V = \text{Volume of water vapor} - \text{Volume of liquid water} ]
Finally, plug in the values into the equation for ( \Delta U ):
[ \Delta U = 40.66 , \text{kJ/mol} - (1.00 , \text{atm}) \times \Delta V ]
Calculate ( \Delta V ): [ \Delta V = 30.6 , \text{L/mol} - \left(\frac{18 , \text{g/mol}}{996 , \text{g/L}}\right) ]
Then, substitute ( \Delta V ) into the equation for ( \Delta U ) and solve for ( \Delta U ).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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