thermodynamics of the internal combustion engine

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Thermodynamics of the Internal Combustion Engine AGUS HARYANTO

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Thermodynamics of the Internal Combustion Engine. AGUS HARYANTO. PERSAMAAN2 TERMODINAMIKA. Hukum Boyle untuk gas ideal: P 1 V 1 = P 2 V 2 = P n V n = konstan Hukum Charles: Pada P konstan , V 1 /V 2 = T 1 /T 2 Pada V konstan , P 1 /P 2 = T 1 /T 2 Persamaan gas ideal - PowerPoint PPT Presentation

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Page 1: Thermodynamics of the Internal Combustion Engine

Thermodynamics of the Internal Combustion Engine

AGUS HARYANTO

Page 2: Thermodynamics of the Internal Combustion Engine

PERSAMAAN2 TERMODINAMIKA

• Hukum Boyle untuk gas ideal:P1V1 = P2V2 = PnVn = konstan

• Hukum Charles:Pada P konstan, V1/V2 = T1/T2

Pada V konstan, P1/P2 = T1/T2

• Persamaan gas idealP1V1/T1 = P2V2/T2 = … PV/T = RPV = RT PV = mRT

Page 3: Thermodynamics of the Internal Combustion Engine

PERNYATAAN Kelvin-Plank (1850)

For heat engines:It is impossible for any

device that operates on a cycle to receive heat from a single reservoir and produce a net amount of work.

Page 4: Thermodynamics of the Internal Combustion Engine

BOTTOM LINE

• Tidak ada mesin siklik yang memiliki efisiensi 100%

Page 5: Thermodynamics of the Internal Combustion Engine

Panas spesifik, entropi, perubahan energi dakhil

• Panas spesifikQ = mCp(T2 – T1)

• EntropiT dS = dQ

• Perubahan energi:Q = U2 – U1 + W

Page 6: Thermodynamics of the Internal Combustion Engine

Diagram P-v dan T-s

Page 7: Thermodynamics of the Internal Combustion Engine

Efisiensi Termal

Page 8: Thermodynamics of the Internal Combustion Engine

cold-air-standard assumptionsAir-standard assumptions: 1. The working fluid is air, which circulates in a

closed loop and behaves as an ideal gas. 2. All the processes are internally reversible. 3. The combustion process is replaced by a heat-

addition from an external source4. The exhaust process is replaced by a heat-

rejection and restores the fluid to initial state.• Air has constant specific heats at room temperature

25°C. cold-air-standard assumptions.

Page 9: Thermodynamics of the Internal Combustion Engine

Siklus Motor Otto (bensin) Ideal

The ideal Otto cycle consists of four internally reversible processes:

• 1-2 Isentropic compression • 2-3 Constant-volume heat addition

(Combustion)• 3-4 Isentropic expansion (Langkah usaha)• 4-1 Constant-volume heat rejection (langkah

buang)

Page 10: Thermodynamics of the Internal Combustion Engine
Page 11: Thermodynamics of the Internal Combustion Engine

ENERGY BALANCE SIKLUS OTTO

• (qin – qout) + (win – wout) = u

• Qin = u3 – u2 = Cv(T3 – T2)

• Qout = u4 – u1 = Cv(T4 – T1)

Page 12: Thermodynamics of the Internal Combustion Engine

ENERGY BALANCE SIKLUS OTTO

• Mean effective pressure (MEP): if it acted on the piston during the entire power stroke, would produce the same amount of net work as that produced during the actual cycle

• Wnet = MEP * Vol. displcm

Page 13: Thermodynamics of the Internal Combustion Engine

ENERGY BALANCE SIKLUS OTTO

• r = compression ratio• k = heat specific ratio = Cp/Cv

Page 14: Thermodynamics of the Internal Combustion Engine

Note: Compression ratio yang tinggi akan berakibat pada suhu kompresi yang tinggi juga. Pada motor bensin, jika suhu ini mengakibatkan AUTOIGNITION dan menghasilkan noise yang disebut KNOCKING. Efisiensi termal motor bensin aktual 25 - 30 %.

Page 15: Thermodynamics of the Internal Combustion Engine

ENERGY BALANCE SIKLUS DIESEL

• (qin – qout) + (wb) = u

• Qin = h3 – h2 = Cp(T3 – T2)

• Qout = u4 – u1 = Cv(T4 – T1)

Page 16: Thermodynamics of the Internal Combustion Engine

ENERGY BALANCE SIKLUS DIESEL

Page 17: Thermodynamics of the Internal Combustion Engine

Note: Eff. Thermal Motor bensin > diesel the same compression ratio. Efisiensi termal motor diesel aktual 35- 40 %.