Problem 26
Question
The internal energy change (in \(\mathrm{J}\) ) when \(90 \mathrm{~g}\) of water undergoes complete evaporation at \(100^{\circ} \mathrm{C}\) is \(.\) (Given : \(\Delta \mathrm{H}_{\text {vap }}\) for water at \(373 \mathrm{~K}=41 \mathrm{~kJ} / \mathrm{mol}, \mathrm{R}=8.314 \mathrm{JK}^{-1} \mathrm{~mol}^{-1}\) )
Step-by-Step Solution
Verified Answer
The internal energy change is 40.5 kJ.
1Step 1: Understand the Problem
The problem involves calculating the internal energy change during the evaporation of water at 100°C. We are given the enthalpy of vaporization and need to find the internal energy change. This can be done using the formula: \[ \Delta U = \Delta H - P\Delta V \]where \( P\Delta V = nR\Delta T \). However, \( \Delta T \) is zero because the process happens at a constant temperature, simplifying to \(P\Delta V = nRT\text{ (only for ideal gas approximation)} \).
Key Concepts
Internal Energy ChangeEnthalpy of VaporizationIdeal Gas Approximation
Internal Energy Change
The change in internal energy, denoted as \( \Delta U \), reflects how much energy is absorbed or released within a system during a process, like the evaporation of water. During a phase change, such as when water transforms from liquid to vapor, energy is needed to overcome intermolecular forces. This energy input does not contribute to a temperature change but rather alters the state of the substance.
In the exercise, we calculate \( \Delta U \) using the formula:
In the exercise, we calculate \( \Delta U \) using the formula:
- \( \Delta U = \Delta H - P\Delta V \)
Enthalpy of Vaporization
Enthalpy of vaporization, \( \Delta H_{\text{vap}} \), is the energy required to convert a substance from a liquid to a gas at constant temperature and pressure. For water, this process occurs at 100°C or 373K, during which each mole of water absorbs heat.
- Given that \( \Delta H_{\text{vap}} = 41 \text{ kJ/mol} \) for water, this value is intrinsic to water's ability to vaporize.
Ideal Gas Approximation
The ideal gas approximation simplifies calculations by assuming certain conditions under which a gas behaves perfectly. For gases, this means they're considered to have:
- Elastic collisions
- No intermolecular forces
- Infinitesimal particle volume
Other exercises in this chapter
Problem 24
In a constant volume calorimeter, \(3.5 \mathrm{~g}\) of a gas with molecular weight 28 was burnt in excess oxygen at \(298.0 \mathrm{~K}\). The temperature of
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At constant volume, \(4 \mathrm{~mol}\) of an ideal gas when heated from \(300 \mathrm{~K}\) to \(500 \mathrm{~K}\) changes its internal energy by \(5000 \mathr
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