The saturated-air enthalpy of the air at the local water temperature, hs(Tw), against the operating line ha(Tw) = hin + (L/G) cp,w (Tw − Tc), with the band between them — the driving force the Merkel integral sums — narrowing toward the cold end.

Reference conditions: cold water 32 °C, hot water 42 °C, entering air 33 °C dry bulb / 27 °C wet bulb, L/G 1.50, cp,w 4.18 kJ/kg·K.

Formula: KaV/L = ∫ cp,w dTw / (hs(Tw) − ha(Tw)) with ha(Tw) = hin + (L/G) cp,w (Tw − Tc).

Merkel demand curve: saturated-air enthalpy against the operating line (illustrative)Illustrative Merkel demand curve for cooling-tower fill. The rising line is the saturation enthalpy of air at the local water temperature, hs(Tw); the straight line is the operating line ha(Tw) = hin + (L/G) cp,w (Tw − Tc). Reference condition: cold water 32 °C, hot water 42 °C, entering air 33 °C dry bulb / 27 °C wet bulb, L/G 1.50, cp,w 4.18 kJ/kg·K. Saturation enthalpy rises from 110.65 kJ/kg at 32 °C to 183.63 kJ/kg at 42 °C; the operating line rises from 85.05 to 147.75 kJ/kg. The gap between them — the driving force the Merkel integral sums as cp,w/(hs − ha) over 32 to 42 °C — is 35.88 kJ/kg at the hot end and 25.60 kJ/kg at the cold end, which is why the last degrees of approach cost the most fill. Values are computed from the formulas, not measured; no tower, no rating. (chart-merkel)Merkel curve — Illustrative — not a measurementSaturated air vs the operating line32343638404280100120140160180Water temperature Tw (°C)Air enthalpy (kJ/kg dry air)25.6035.88Reference condition: water 32–42 °C · entering air 33 °C db / 27 °C wbL/G1.50cp,w (kJ/kg·K)4.18slope (L/G)·cp,w (kJ/kg·K)6.27gap hs − ha (kJ/kg)25.60 – 35.88Computed from the formula — not field data.
Illustrative, computed from the formulas above — not a measurement. The rising line is the saturated-air enthalpy the integral sums against; the straight line is the operating line at the reference condition, and the hatched band between them is the driving force.

Sources