Concept:
The dew point temperature (\( T_{dp} \)) of a moist air mixture is defined as the temperature to which the air must be cooled at a constant total pressure to reach full saturation (\( \text{Relative Humidity} = 100\% \)). At this point, the initial condensation of liquid water begins. Thermodynamically, the dew point temperature depends uniquely on the partial pressure of water vapor (\( p_v \)) present in the mixture.
Step 1: Linking absolute humidity to partial pressure.
Let us evaluate the relationship between absolute humidity (also called humidity ratio, denoted as \( Y \)) and the partial pressure of water vapor (\( p_v \)) in a gas mixture at a total system pressure \( P \):
\[
Y = 0.622 \cdot \frac{p_v}{P - p_v}
\]
Rearranging this algebraic equation to isolate the partial pressure term \( p_v \) yields:
\[
p_v = \frac{Y \cdot P}{0.622 + Y}
\]
This relation shows that at a constant total system operating pressure \( P \), the partial pressure of water vapor \( p_v \) is a monotonically increasing function of the absolute humidity \( Y \):
\[
Y \uparrow \quad \Rightarrow \quad p_v \uparrow
\]
Step 2: Connecting partial pressure to the dew point temperature.
By definition, when a gas mixture cools to its dew point temperature, the partial pressure of water vapor matches the saturation vapor pressure of pure water at that specific temperature:
\[
p_v = p_{sat}(T_{dp})
\]
According to the Clausius-Clapeyron equation, the saturation pressure of water increases monotonically with temperature:
\[
T_{dp} \uparrow \quad \Longleftrightarrow \quad p_{sat}(T_{dp}) \uparrow
\]
Since an increase in absolute humidity (\( Y \)) increases the partial pressure of water vapor (\( p_v \)), it requires a higher saturation temperature to initiate condensation.
Therefore, if the absolute humidity of an air-water vapor mixture increases, its dew point temperature increases accordingly.