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Marine Propulsion & Diesel Engines

Theoretical Cycles — Otto, Diesel & Dual Combustion

Three ideal heat-addition stories on one p-V plot — and why real marine diesels follow the dual one.

6 min read
Beginner
Marine Propulsion & Diesel Engines
Key Principles at a Glance 5 points
  • All three cycles assume air as an unchanging working fluid with no induction or exhaust strokes — heat simply appears and disappears.
  • Otto adds all heat at constant volume (2–3 vertical); Diesel adds all heat at constant pressure (2–3 horizontal).
  • Dual splits the difference: part of the heat at constant volume, the rest at constant pressure — closest to real diesel burning.
  • Every cycle closes the same way: isentropic expansion for work, then constant-volume heat rejection back to the start.
  • No real engine follows any of them strictly — valve events, finite burn time and heat losses reshape every corner.

1. The Ground Rules All Three Share

Theory strips the engine to its thermodynamic skeleton: a fixed mass of air, compressed and expanded isentropically, with heat added at one stage and rejected at another. Induction and exhaust strokes do not exist in this world — the cycle is a closed loop, and efficiency depends only on how the heat is added and how far the air expands.

CLOSED LOOP — NO INDUCTION, NO EXHAUST COMPRESS HEAT IN EXPAND REJECT

2. Otto — All Heat at Constant Volume

Compress air isentropically (1–2), dump all heat in with the piston parked (2–3, vertical line — volume frozen, pressure leaping), expand isentropically (3–4), reject heat at constant volume (4–1). Instantaneous burning at top dead centre is the idealisation — and the petrol engine's theoretical home.

OTTO — HEAT AT FIXED VOLUME 1-2 COMPRESS HEAT V const 3-4 EXPAND 4-1 REJECT
Otto cycle p-V diagram with vertical constant-volume heat addition
Figure 1: Otto — read the vertical 2–3: heat in, piston unmoved.

3. Diesel — All Heat at Constant Pressure

Same isentropic compression (1–2), but heat enters while the piston retreats just fast enough to hold pressure steady (2–3, horizontal line) — slow, controlled burning as in early air-blast diesels. Then isentropic expansion (3–4) and constant-volume rejection (4–1) exactly as before.

DIESEL — HEAT AT FIXED PRESSURE 1-2 COMPRESS HEAT p const 3-4 EXPAND 4-1 REJECT
Diesel cycle p-V diagram with horizontal constant-pressure heat addition
Figure 2: Diesel — read the horizontal 2–3: heat in, pressure held.

4. Dual — the Marine Diesel Compromise

Real fuel burns in two phases: a rapid premixed spike near constant volume, then a drawn-out diffusion burn near constant pressure. The dual cycle writes exactly that — heat partly at constant volume (2–3), partly at constant pressure (3–4) — followed by adiabatic expansion to point 5 and constant-volume rejection home. This is the cycle modern marine diesels are analysed against.

DUAL — SPLIT HEAT, VOLUME THEN PRESSURE HEAT AT V HEAT AT p EXPAND REJECT
Dual combustion p-V diagram with heat added first at constant volume then at constant pressure
Figure 3: Dual — heat in two instalments, matching how fuel really burns.
CycleHeat addedDescribes
OttoConstant volumePetrol / gas engines
DieselConstant pressureEarly slow-burn oil engines
DualVolume then pressureModern marine diesels