I. THERMODYNAMIC CYCLES
A. Spark Ignition (SI) Engine Cycles
1. Ideal Otto Cycle
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Processes:
1-2: Isentropic compression
2-3: Constant volume heat addition
3-4: Isentropic expansion
4-1: Constant volume heat rejection
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Assumptions: Air as ideal gas, constant specific heats, no friction, reversible processes, no pressure drops.
-
P-V and T-S Diagrams:
DiagramSEARCH: Otto cycle PV TS diagram -
Air Standard Efficiency:
$$\eta = 1 - \frac{1}{r^{\gamma-1}}$$
where \(r\) = compression ratio, \(\gamma = C_p/C_v\).
- Work Output: \(W = Q_{in} - Q_{out} = C_v(T_3 - T_2) - C_v(T_4 - T_1)\).
2. Otto Cycle Calculations
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Given initial conditions (\(P_1, T_1\)), compression ratio \(r\), heat added \(Q_{in}\):
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\(T_2 = T_1 r^{\gamma-1}\), \(P_2 = P_1 r^\gamma\)
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\(T_3 = T_2 + Q_{in}/C_v\)
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\(P_3 = P_2 (T_3/T_2)\) (constant volume)
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\(T_4 = T_3 / r^{\gamma-1}\), \(P_4 = P_3 / r^\gamma\)
-
-
Mean Effective Pressure (MEP):
$$MEP = \frac{W}{V_s} = \frac{Q_{in} \left(1 - \frac{1}{r^{\gamma-1}}\right)}{V_1 \left(1 - \frac{1}{r}\right)}$$
where \(V_s = V_1 - V_2\) (swept volume).
3. Actual Otto Cycle Deviations
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Variation of specific heats (\(\gamma\) decreases with temperature).
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Pressure drops in intake/exhaust manifolds.
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Heat transfer to cylinder walls.
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Friction and pumping losses.
[!TIP] In calculations, use absolute temperature (K) and consistent units.
B. Compression Ignition (CI) Engine Cycles
1. Ideal Diesel Cycle
-
Processes:
1-2: Isentropic compression
2-3: Constant pressure heat addition
3-4: Isentropic expansion
4-1: Constant volume heat rejection
-
P-V and T-S Diagrams:
DiagramSEARCH: Diesel cycle PV TS diagram -
Cut-off ratio: \(\alpha = V_3 / V_2\).
2. Diesel Cycle Analysis
- Efficiency:
$$\eta = 1 - \frac{1}{r^{\gamma-1}} \left( \frac{\alpha^\gamma - 1}{\gamma(\alpha - 1)} \right)$$
- For same compression ratio \(r\) and same heat input, Otto cycle is more efficient because heat addition at constant volume yields higher average temperature.
3. Diesel Cycle Calculations
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Given \(r\), \(\alpha\), \(P_1, T_1\):
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\(T_2 = T_1 r^{\gamma-1}\), \(P_2 = P_1 r^\gamma\)
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\(T_3 = T_2 + Q_{in}/C_p\) (since constant pressure, \(P_3 = P_2\))
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\(V_3 = \alpha V_2\), so \(T_3 = T_2 \alpha\) (from ideal gas law)
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\(T_4 = T_3 / r^{\gamma-1}\)
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Efficiency from formula above.
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C. Dual Cycle (Mixed Cycle)
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Heat addition partly at constant volume (2-3) and partly at constant pressure (3-4).
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More realistic than Otto or Diesel alone.
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Efficiency lies between Otto and Diesel for same \(r\).
D. Cycle Comparisons
| Comparison Basis | Otto | Diesel | Dual |
|---|---|---|---|
| Same compression ratio | Higher efficiency | Lower efficiency | Intermediate |
| Same maximum pressure | Lower compression ratio possible | Higher compression ratio possible | Depends on cut-off ratio |
| Same heat input | Higher max temperature | Lower max temperature | Intermediate |
II. ENGINE CYCLE ANALYSIS AND PERFORMANCE PARAMETERS
A. Actual vs Ideal Engine Cycles
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Theoretical Valve Timing: Intake opens at TDC, closes at BDC; exhaust opens at BDC, closes at TDC.
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Actual Valve Timing:
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Intake opens before TDC (lead), closes after BDC (lag).
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Exhaust opens before BDC, closes after TDC.
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Overlap period: Both valves open (intake and exhaust).
DiagramSEARCH: actual valve timing diagram 4 stroke -
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Causes of Deviation:
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Flow losses (pressure drops in ports, valves).
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Heat transfer to walls.
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Friction and accessory drives.
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B. Performance Parameters and Definitions
| Parameter | Definition | Formula |
|---|---|---|
| Indicated Power (IP) | Power developed in cylinder from pressure-volume work | \(IP = \frac{IP_{cyl} \times n \times N}{60}\) (for 4-stroke, cycles/min = N/2) |
| Brake Power (BP) | Power available at output shaft (dynamometer) | \(BP = \frac{2\pi T N}{60}\) (T in N·m, N in rpm) |
| Mechanical Efficiency | \(\eta_m = \frac{BP}{IP}\) | |
| Indicated Thermal Efficiency | \(\eta_{ith} = \frac{IP}{\dot{m}_f Q_{HV}}\) | |
| Brake Thermal Efficiency | \(\eta_{bth} = \frac{BP}{\dot{m}_f Q_{HV}}\) | |
| Volumetric Efficiency | \(\eta_v = \frac{\text{Actual air intake}}{\text{Swept volume at intake conditions}}\) | Factors: clearance volume, valve timing, intake tuning (resonance), temperature, pressure drop. |
| Specific Fuel Consumption (SFC) | BSFC = \(\frac{\dot{m}_f}{BP}\), ISFC = \(\frac{\dot{m}_f}{IP}\) | |
| Mean Effective Pressure (MEP) | Hypothetical pressure that, if acted on piston during power stroke, would produce same work | Indicated MEP: \(IMEP = \frac{IP \times 60}{n \times N \times V_s}\) (4-stroke) <br> Brake MEP: \(BMEP = \frac{BP \times 60}{n \times N \times V_s}\) |
C. Engine Testing and Performance Calculation
1. Morse Test (for multi-cylinder engines)
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Method:
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Run all cylinders, measure BP\(_{all}\).
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Cut out one cylinder at a time, measure BP\(_i\) for remaining cylinders.
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Assumptions:
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Friction power of each cylinder is identical.
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Friction power of cut-out cylinder remains constant when cut.
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Calculations:
$$IP = \frac{n \cdot BP_{all} - \sum_{i=1}^{n} BP_i}{n-1}$$
$$\eta_m = \frac{BP_{all}}{IP}$$
where \(n\) = number of cylinders.
2. Heat Balance Sheet
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Energy Input: \(\dot{Q}_{in} = \dot{m}_f \times CV\) (kJ/min or kJ/s).
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Energy Output Distribution:
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Brake Power (BP)
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Heat to cooling water: \(\dot{Q}_w = \dot{m}_w C_{pw} \Delta T_w\)
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Heat to exhaust gases: \(\dot{Q}_{ex} = \dot{m}_{ex} C_{pex} (T_{ex} - T_{amb})\)
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Heat to radiation & unaccounted: \(\dot{Q}_{rad} = \dot{Q}_{in} - (BP + \dot{Q}_w + \dot{Q}_{ex})\)
-
-
Preparation: All quantities on per minute or per second basis. Sum of outputs ≈ input (allow 5% error).
3. Performance Calculation from Trial Data
-
Given: Torque \(T\), speed \(N\), fuel consumption \(\dot{m}_f\), air consumption \(\dot{m}_a\), cooling water data, exhaust gas data, calorific value \(CV\).
-
Steps:
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\(BP = \frac{2\pi T N}{60}\)
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\(BSFC = \frac{\dot{m}_f}{BP}\)
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\(\eta_{bth} = \frac{BP}{\dot{m}_f CV}\)
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Heat balance as above.
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III. COMBUSTION IN SPARK IGNITION (SI) ENGINES
A. Stages of Combustion (with Pressure-Crank Angle Diagram)
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Ignition Delay (Lag):
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Physical phase: Fuel atomization, vaporization, mixing with air.
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Chemical phase: Pre-flame reactions (low-temperature oxidation).
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Flame Propagation:
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Initial stage: Flame kernel growth (0–10° after spark).
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Main stage: Turbulent flame spread (10–80% of charge).
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Afterburn: Combustion of remaining charge near walls.
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Rates:
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Rate of pressure rise: \(\frac{dp}{d\theta}\) (max during main combustion).
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Rate of combustion: \(\frac{dQ}{d\theta}\).
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B. Factors Affecting Flame Speed
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Turbulence/Swirl/Squish: Increase flame speed (turbulent flame speed \(S_T \gg\) laminar \(S_L\)).
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Compression ratio: Higher \(r\) → higher \(T, P\) → faster flame.
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Fuel-air ratio: Stoichiometric (\(\phi=1\)) gives maximum flame speed.
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Temperature & Pressure: Higher intake \(T, P\) increase flame speed.
C. Abnormal Combustion
1. Detonation/Knock
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Phenomenon: Spontaneous ignition of end gas ahead of flame front, causing high-frequency pressure waves ("pinging").
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Theories:
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Thermal theory: Hot spots (e.g., carbon deposits) initiate combustion.
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Pressure wave theory: Pressure waves compress end gas to auto-ignition.
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Chemical theory: Low-temperature oxidation reactions.
-
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Effects: Power loss, overheating, piston damage, bearing failure.
2. Variables Affecting Detonation
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High compression ratio.
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Advanced ignition timing.
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Low octane rating fuel.
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High intake temperature/pressure.
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Carbon deposits in combustion chamber.
3. Pre-ignition
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Cause: Fuel ignites before spark (due to hot spots like glowing deposits, spark plug overheating).
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Difference from detonation: Pre-ignition occurs before spark; detonation after spark but abnormal.
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Remedy: Retard ignition timing, use higher octane fuel, clean deposits, select correct spark plug heat range.
4. Knock Comparison: SI vs CI
| Aspect | SI Engine | CI Engine |
|---|---|---|
| Timing | After spark (end gas) | After injection start (delay period) |
| Cause | Auto-ignition of homogeneous mixture | Sudden combustion of fuel accumulated during delay |
| Dependency | Octane number | Cetane number (inverse) |
5. Control of Abnormal Combustion
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Fuel additives (tetraethyl lead, MTBE, aromatics).
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Design changes: swirl/tumble, squish, compact chamber.
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Ignition timing retardation.
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Cooling of intake charge.
D. Combustion Chamber Design for SI Engines
1. Desirable Characteristics
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Compact (short flame travel).
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High turbulence/swirl at TDC.
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Proper squish clearance (0.5–1.5 mm).
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No sharp corners (avoid hotspots).
2. Types of Combustion Chambers
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Shallow piston bowl: Simple, but moderate turbulence.
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Hemispherical (Hemi): Large valves, good breathing, high compression, but heavy.
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Wedge: Simple, good turbulence, used in American V8s.
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Pentroof: Modern, multi-valve, high turbulence, compact.
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Swirl/Tumble chambers: Pre-combustion chambers for high turbulence.
3. Shape Effects: Compact shape reduces knock; high turbulence increases flame speed, reduces knock tendency.
E. Ignition Systems
1. Ignition Lag: Decreases with higher intake temperature/pressure, turbulence, and advanced timing.
2. Spark Plug Requirements
-
Heat range: Cold plug (fast heat transfer) for high-performance engines; hot plug for low-speed to avoid fouling.
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Gap: 0.6–1.2 mm (larger gap → stronger spark but higher voltage needed).
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Materials: Nickel, platinum, iridium (long life).
3. Battery Ignition System
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Construction: Battery → ignition switch → coil (primary/secondary) → distributor (points, capacitor) → spark plugs.
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Working: Points open/close primary current, inducing high voltage in secondary.
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Advantages: Simple, cheap.
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Disadvantages: Points wear, limited spark energy at high speed, maintenance.
4. Electronic Ignition: Transistor/contactless triggering, longer life, better spark, no maintenance.
IV. COMBUSTION IN COMPRESSION IGNITION (CI) ENGINES
A. Stages of Combustion
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Ignition Delay Period:
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Physical phase: Atomization, evaporation, mixing of fuel with air.
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Chemical phase: Pre-flame reactions (low-temperature oxidation).
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Rapid Combustion (Uncontrolled): Combustion of fuel accumulated during delay → rapid pressure rise.
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Controlled Combustion (Diffusion): Fuel burns as it mixes with air (controlled by injection rate).
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Afterburning: Late combustion near exhaust valve.
B. Factors Affecting Delay Period
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Fuel Properties:
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Cetane number: Higher cetane → shorter delay.
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Volatility & viscosity: Higher volatility → shorter delay.
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Engine Conditions:
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Higher compression ratio → higher \(T, P\) → shorter delay.
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Higher intake temperature/pressure → shorter delay.
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Load: Higher load → higher \(T, P\) → shorter delay.
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Injection Parameters:
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Start of injection timing (advanced → longer delay? Actually, advanced injection gives more time for mixing, but delay period itself may shorten with higher \(T, P\)).
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Spray pattern & atomization: Better atomization → shorter delay.
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C. Fuel Injection Systems
1. Functions:
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Metering: Correct quantity of fuel.
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Timing: Start and duration of injection.
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Atomization: Break fuel into fine droplets.
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Distribution: Proper spray pattern in cylinder.
2. Types of Injection Systems
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Air injection (obsolete): Air carries fuel into cylinder.
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Solid injection:
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Common rail: High-pressure accumulator, electronically controlled injectors.
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Unit injector: Pump and nozzle per cylinder, cam-driven.
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Pump-line-nozzle: Inline or distributor pump, high-pressure lines, nozzle.
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3. Fuel Injector (Nozzle)
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Construction: Body, needle valve, spring, orifice.
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Working: High-pressure fuel lifts needle, sprays through orifices.
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Types:
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Hole type: Multiple holes, common in direct injection.
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Pintle type: Pintle valve extends, better atomization, used in indirect injection.
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Throttle type: For specific spray patterns.
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D. Combustion Chambers for CI Engines
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Open chamber (direct injection): High compression ratio, efficient, requires high injection pressure.
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Pre-combustion chamber: Auxiliary chamber connected by orifice, easier starting, smoother.
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Swirl chamber: Auxiliary chamber with tangential entry, creates swirl, good mixing.
E. Diesel Knock
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Phenomenon: Violent noise due to sudden pressure rise when combustion starts after long delay.
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Relation to delay period: Longer delay → more fuel accumulated → faster combustion → higher pressure rise → more knock.
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Cetane number: Higher cetane → shorter delay → less knock.
V. FUEL SYSTEMS AND MIXTURE PREPARATION
A. Carburetion in SI Engines
1. Definition: Formation of homogeneous air-fuel mixture for SI engine.
2. Theory of Carburetion
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Based on Bernoulli's principle: Velocity increase → pressure drop.
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Venturi effect: Throat area \(A_t\), pressure drop \(\Delta P = P_0 - P_t\).
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Air flow velocity: \(v_a = \sqrt{\frac{2\Delta P}{\rho_a}}\).
3. Simple Carburetor
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Components: Float chamber (maintains fuel level), venturi, fuel jet, throttle valve.
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Working: Air flows through venturi → pressure drop at fuel jet → fuel sucked from float chamber.
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Float chamber venting: Ventilated to atmosphere to maintain atmospheric pressure in float chamber; otherwise, fuel flow would be affected by altitude changes.
4. Limitations of Simple Carburetor
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No compensation for engine speed/load.
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Poor mixture at part load.
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No altitude compensation.
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Backfire risk.
5. Carburetor Circuits
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Float circuit: Maintains fuel level.
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Idle circuit: Low throttle operation.
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Main circuit: Normal operation.
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Power circuit: Acceleration enrichment.
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Choke: Cold start enrichment.
6. Carburetor Calculations
- Air flow rate (compressible flow through venturi):
$$\dot{m}_a = C_d A_t P_0 \sqrt{\frac{2\gamma}{R(\gamma-1)}\left[\left(\frac{P_t}{P_0}\right)^{2/\gamma} - \left(\frac{P_t}{P_0}\right)^{(\gamma+1)/\gamma}\right]}$$
where \(P_t = P_0 - \Delta P\), \(C_d\) = discharge coefficient.
- Fuel flow rate:
$$\dot{m}_f = C_f A_f \sqrt{2\rho_f (P_t - P_{fuel} - \rho_f g h)}$$
\(h\) = fuel head (vertical distance from fuel surface to jet).
-
Air-Fuel Ratio: \(A/F = \dot{m}_a / \dot{m}_f\).
-
With nozzle lip considered: Effective pressure at fuel orifice reduced by dynamic pressure of air:
$$\dot{m}_f = C_f A_f \sqrt{2\rho_f (P_t - P_{fuel} - \rho_f g h - \frac{1}{2}\rho_a v_a^2)}$$
7. Mixture Types
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Rich: \(A/F < 14.7:1\) (gasoline), more fuel, cooler, incomplete combustion.
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Stoichiometric: \(A/F \approx 14.7:1\), ideal for catalytic converter.
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Lean: \(A/F > 14.7:1\), less fuel, hotter, better economy but risk of mis-fire.
B. Multi-Point Fuel Injection (MPFI)
-
System: Injector per cylinder, located near intake valve; electronic control (ECU) based on sensors.
-
Merits over carburetor:
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Accurate metering per cylinder.
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Better fuel economy & emissions.
-
No throttle losses (in some systems).
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Better cold-start performance.
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Demerits: Higher cost, complexity, maintenance.
VI. FUELS AND ALTERNATIVE FUELS
A. Chemical Composition of Fuels
| Type | General Formula | Saturation | Structure |
|---|---|---|---|
| Paraffins (Alkanes) | \(C_nH_{2n+2}\) | Saturated | Straight/branched chains |
| Olefins (Alkenes) | \(C_nH_{2n}\) | Unsaturated | One double bond |
| Naphthenes (Cycloalkanes) | \(C_nH_{2n}\) | Saturated | Cyclic rings |
| Aromatics | \(C_nH_n\) (or with substituents) | Unsaturated | Benzene rings |
B. Fuel Ratings
1. Octane Number (SI Engines)
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Definition: Percentage by volume of iso-octane in mixture with n-heptane that matches knocking tendency of test fuel.
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RON (Research Octane Number): Mild test conditions.
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MON (Motor Octane Number): Severe test conditions (higher engine speed, temperature).
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Anti-knock Index (AKI): \((\text{RON} + \text{MON})/2\).
2. Cetane Number (CI Engines)
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Definition: Percentage by volume of cetane (hexadecane) in mixture with heptamethylnonane that matches ignition delay of test fuel.
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Higher cetane → shorter ignition delay → smoother combustion.
-
Measured in standard CFR engine.
C. Desirable Fuel Characteristics
| SI Engines | CI Engines |
|---|---|
| High octane number | High cetane number |
| Good volatility (easy vaporization) | Moderate volatility (avoid vapor lock) |
| Clean burning (low deposits) | Low smoke tendency |
| Resistance to pre-ignition | Good cold-start properties |
D. Alternative Fuels (Frequent)
1. Gaseous Fuels
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CNG (Compressed Natural Gas): Mainly methane, high octane (~120), clean, low CO₂, but low energy density, requires high-pressure cylinders.
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LPG (Liquefied Petroleum Gas): Propane/butane, high octane, clean, stored as liquid under pressure.
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Biogas: Methane from biomass, similar to CNG but may contain CO₂, H₂S.
2. Hydrogen
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Properties: Wide flammability limits (4–75%), high flame speed, low density, high auto-ignition temperature.
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Usage in SI: Can be used with modifications (higher compression, hardened valves).
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Usage in CI: Dual-fuel (pilot diesel ignition), or hydrogen-diesel co-combustion.
3. Biofuels
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Ethanol: From biomass, high octane, oxygenated, reduces CO, but hydrophilic, lower energy density, corrosion.
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Biodiesel: From vegetable oils/animal fats, similar to diesel, lower emissions (except NOx), can cause filter plugging.
4. Summary for SI and CI
| Fuel | SI Suitability | CI Suitability |
|---|---|---|
| CNG/LPG | Excellent (high octane) | Possible with dual-fuel |
| Hydrogen | Good (high octane) | Possible with pilot injection |
| Ethanol | Excellent (high octane) | Not suitable (low cetane) |
| Biodiesel | Not suitable (low octane) | Excellent (good cetane) |
E. Fuel Additives (Dopes)
1. Purpose:
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Improve combustion (octane/cetane boosters).
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Reduce emissions (detergents, smoke suppressants).
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Protect engine (corrosion inhibitors, antioxidants).
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Improve storage stability (anti-oxidants, metal deactivators).
2. Requirements of Good Additive:
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Effective at low concentration.
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Compatible with fuel and engine materials.
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Stable under storage and operating conditions.
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Non-corrosive, non-toxic.
3. Types:
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Antioxidants: Prevent gum formation (e.g., phenolic compounds).
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Anti-knock agents: Increase octane (e.g., tetraethyl lead [banned], MTBE, ETBE, aromatics).
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Detergents: Keep injectors/valves clean (e.g., polyisobutene amine).
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Cetane improvers: Alkyl nitrates (e.g., 2-ethylhexyl nitrate).
4. Knock Inhibitors:
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Lead-based (historical): Tetraethyl lead (TEL).
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Oxygenates: MTBE, ETBE, alcohols.
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Aromatics: Benzene, toluene (limited due to emissions).
VII. SUPERCHARGING AND TURBOCHARGING
A. Need for Supercharging
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Increase power output without increasing engine size.
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Improve torque at low speeds.
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Compensate for altitude loss (aircraft engines).
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Enhance acceleration.
B. Effect on Engine Performance
| Aspect | Effect |
|---|---|
| Power output | Increases (more air → more fuel → more power) |
| Fuel consumption | Brake specific fuel consumption may decrease (better efficiency) but total fuel rate increases. |
| Thermal efficiency | SI: May decrease due to higher \(T_{max}\) and knock; CI: May increase due to better combustion. |
| Detonation tendency (SI) | Increases due to higher pressure and temperature. |
| Mechanical stress | Increases (higher pressures, temperatures, forces). |
C. Methods of Supercharging
1. Positive Displacement Superchargers
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Roots: Two meshing lobes, positive displacement, boost at low rpm, inefficient at high speed.
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Vane: Rotor with sliding vanes, smoother but wear issues.
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Twin-screw: Two meshing screws, high efficiency, compact.
2. Dynamic Superchargers (Centrifugal)
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Impeller accelerates air, diffuser converts velocity to pressure.
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Boost increases with rpm (lag at low speed).
3. Turbocharging
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Need: Utilize exhaust gas energy, improve efficiency.
-
Methods:
-
Constant pressure: All exhaust gases combined into single turbine (simple, but pulse energy lost).
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Pulse turbocharging: Exhaust pulses from individual cylinders directed to turbine (utilizes pulse energy, more efficient).
-
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Merits: No parasitic loss (uses waste energy), high efficiency.
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Demerits: Turbo lag, high exhaust backpressure, heat, complexity.
D. Thermodynamic Cycle of Supercharged Engine
-
Intake pressure > atmospheric → higher mass of air per cycle.
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Net work increases, but compression work may increase if supercharger is driven mechanically.
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For turbocharged, exhaust energy recovery improves overall efficiency.
E. Limitations of Supercharging
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SI Engines:
-
Knock limit: Maximum pressure/temperature before knock.
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Mechanical limits: Piston, connecting rod strength.
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-
CI Engines:
-
Pressure limits: Fuel injection system must handle higher pressures.
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Smoke limit: Air availability may become insufficient at high loads.
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VIII. ENGINE COOLING SYSTEMS
A. Need for Cooling
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Prevent overheating and seizure.
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Maintain efficient operation (optimal temperature ~80–100°C).
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Reduce detonation tendency in SI engines.
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Ensure proper lubrication (oil viscosity).
B. Types of Cooling Systems
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Air Cooling: Fins on cylinder/head, airflow from vehicle motion or fan. Simple, no coolant, but uneven cooling.
-
Liquid Cooling: Coolant (water/antifreeze) circulated through jackets, radiator dissipates heat.
-
Forced Cooling System (most common):
DiagramSEARCH: engine forced liquid cooling system diagram-
Components: Water pump, thermostat, radiator, fan, coolant passages.
-
Working: Pump circulates hot coolant to radiator → cooled by air → returns to engine. Thermostat regulates flow to maintain operating temperature.
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C. Cooling System Components
-
Radiator: Heat exchanger (tubes + fins).
-
Cooling Fins: Increase surface area on air-cooled engines.
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Water Pump: Centrifugal type, driven by belt.
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Thermostat: Wax-pellet type, opens at ~80°C.
-
Fan: Mechanical or electric, draws air through radiator.
D. Coolants
-
Anti-freeze Solutions:
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Ethylene glycol (toxic) or propylene glycol (less toxic).
-
Lower freezing point, raise boiling point, inhibit corrosion.
-
-
Additives: Corrosion inhibitors (phosphates, silicates), anti-foaming agents.
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Selection & Maintenance:
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Concentration 30–50% glycol in water.
-
Periodic flushing, check for leaks, test freeze point.
-
IX. ENGINE LUBRICATION SYSTEMS
A. Functions of Lubrication
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Reduce friction and wear.
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Seal piston rings against cylinder wall.
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Cool moving parts (carry heat away).
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Clean (carry contaminants to filter).
-
Prevent corrosion.
B. Properties of Lubricating Oil
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Viscosity: Appropriate for temperature range (SAE grades).
-
Pour point: Lowest temperature for flow.
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Flash point: Minimum temperature for ignition (safety).
-
Carbon residue: Tendency to form deposits.
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Acidity: Low acid number to prevent corrosion.
-
Demulsibility: Ability to separate from water.
C. Types of Lubrication Systems
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Splash Lubrication: Moving parts (e.g., connecting rod) dip in oil and splash around. Used in small engines.
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Pressure Feed (Forced):
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Oil pump supplies pressurized oil to main bearings, camshaft, etc.
-
Full-flow filter filters all oil.
-
DiagramSEARCH: engine pressure lubrication system diagram
-
-
Mist Lubrication: Oil mixed with air, used in 2-stroke engines (oil injected into intake).
-
Dry Sump vs Wet Sump:
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Wet sump: Oil stored in pan, pump picks up oil. Simple but oil sloshes.
-
Dry sump: External tank, scavenge pumps, no oil in sump. Better for high-performance, reduces foaming.
-
D. Lubrication System Sketch
X. EMISSIONS AND CONTROL SYSTEMS
A. Exhaust Gas Recirculation (EGR)
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Purpose: Reduce NOx emissions by lowering combustion temperature.
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Construction & Working:
-
Internal EGR: Exhaust gases routed back via valve in intake manifold.
-
External EGR: Separate cooler and valve, more control.
-
Working: Inert exhaust gases displace air → lower oxygen → lower peak temperature → less NOx.
-
-
Advantages: Effective NOx reduction, relatively simple.
-
Limitations: Increases soot (especially in CI), reduces efficiency, requires cooling to avoid intake heating, may cause drivability issues.
B. Scavenging in 2-Stroke Engines
-
Need: Efficiently remove exhaust gases and fill cylinder with fresh charge (no separate intake stroke).
-
Types:
DiagramSEARCH: 2 stroke engine scavenging types cross loop uniflow-
Cross scavenging: Transfer and exhaust ports on opposite sides, baffles direct flow. Simple but some short-circuiting.
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Loop scavenging: Transfer ports angled, creates looped flow, better scavenging.
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Uniflow scavenging: Exhaust valve at top, inlet at bottom, unidirectional flow (most efficient, used in large marine engines).
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Scavenging Efficiency: Ratio of fresh charge retained to total cylinder volume.
XI. ADVANCED ENGINE CONCEPTS AND MISCELLANEOUS
A. 2-Stroke vs 4-Stroke Engines
| Aspect | 2-Stroke | 4-Stroke |
|---|---|---|
| Power strokes | Every revolution | Every two revolutions |
| Power/weight | Higher (more power per size) | Lower |
| Fuel efficiency | Lower (short expansion, scavenging losses) | Higher |
| Emissions | Higher (oil in fuel, incomplete scavenging) | Lower |
| Complexity | Simpler (no valve train) | More complex (valves, camshaft) |
| Applications | Small engines (motorcycles, lawn mowers) | Automobiles, trucks |
B. Wankel Engine
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Construction: Triangular rotor in epitrochoid chamber, no pistons.
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Working: Rotor's motion creates expanding/contracting volumes; intake, compression, power, exhaust in separate zones.
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Advantages: Compact, smooth (no reciprocating mass), high rpm, high power/weight.
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Disadvantages: Poor fuel economy (large surface/volume ratio, heat loss), high emissions, apex seal wear, poor low-speed torque.
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DiagramSEARCH: Wankel rotary engine diagram
C. Cylinder Arrangement
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In-line: All cylinders in a row. Simple, good for 4-6 cylinders.
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V-type: Two banks angled (e.g., 60°, 90°). Shorter, rigid, used in 6+ cylinders.
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Opposed (Flat): Horizontally opposed cylinders. Low center of gravity, smooth (e.g., Subaru, Porsche).
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Radial: Cylinders arranged radially around crankshaft. Used in aircraft (good cooling, smooth).
D. Microprocessor-Based Control Systems
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Advantages:
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Precise control of fuel injection, ignition timing, emissions.
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Adaptive to conditions (altitude, temperature).
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Onboard diagnostics (OBD).
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Improved fuel economy and performance.
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Disadvantages:
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High cost and complexity.
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Susceptible to electromagnetic interference.
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Requires skilled maintenance.
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Dependency on sensors (failure leads to poor performance).
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\boxed{\eta_{Otto} = 1 - \frac{1}{r^{\gamma-1}}}
\boxed{\eta_{Diesel} = 1 - \frac{1}{r^{\gamma-1}} \left( \frac{\alpha^\gamma - 1}{\gamma(\alpha - 1)} \right)}
\boxed{IP_{Morse} = \frac{n \cdot BP_{all} - \sum BP_i}{n-1}}
\boxed{MEP = \frac{Work\ per\ cycle}{Swept\ volume}}