Condenser condition. Flat & low is good — 16 °C means clean.
Suction & freeze margin — keep above 4.5 bar g.
High side. Rises with sea temperature; fine while approach stays low.
Delivered temperature against the 10 °C setpoint.
The main driver of high-side pressure.
Approach = saturated condensing temp − sea-water outlet. The cleanest measure of how well the condenser sheds heat, with sea temperature taken out. Flat and low is healthy; a sustained climb toward 16 °C is fouling.
The shaded band is the gap between saturated condensing temp (top) and sea-water outlet (bottom) — that gap is the approach.
Sea-water temperature entering and leaving the condenser. The spread between them is how much heat the seawater is carrying away.
Low-side suction pressure. It sets evaporator temperature and the freeze margin. Below 4.5 bar g the plate evaporator is at freezing risk.
Degrees of subcooling at the liquid line. A few degrees confirms a solid liquid seal and adequate charge.
Temperature rise of the sea water across the condenser — the heat actually being rejected overboard.
Chilled-water supply temperature — what the plant actually delivers. It should sit near 10 °C.
Chilled-water return minus supply — the load the ship puts on the plant. It sits flat around 2–2.6 °C.
Each dot is one reading: sea-water inlet (x) against approach (y). A clean condenser holds a flat low band whatever the inlet temperature.
Sea-water inlet (x) against HP (y). Healthy, this is a tight rising line — HP simply following sea temperature.
| bar g | °C | bar g | °C | bar g | °C |
|---|
Corrected Honeywell basis (45 °C ≈ 19 bar g). Mean saturated condensing temperature; R449A glide ~5 K gives ±~2.5 °C. High side only — this is what the approach calculation uses.
Approach = saturated condensing temp (from HP) − sea-water outlet. Same method as the live sheet, so the number matches the log to the decimal.