An air-standard Otto cycle operates with 300 ๐พ and 95 kPa at the start of theย
compression stroke. The compression ratio is 9.5 and the maximum temperature ofย
the cycle is 1100 K. On the basis of a cold air-standard analysis, using ๐๐ฃ =
0.718
๐๐ฝ
๐๐โ๐พ
and ๐๐ = 1.005
๐๐ฝ
๐๐
โ๐พ
, determine theย
(a) temperature at the end of the compression stroke, in K
(b)peak pressure, in kPa
(c) Heat Addition, kJ/kg
(d) net work of the cycle, kJ/kg
(e)thermal Efficiencyย
Q163246
ย Deadline:ย 16.02.21, 04:18
An air-standard Otto cycle operates with 300 ๐พ and 95 kPa at the start of the compression stroke. The compression ratio is 9.5 and the maximum temperature of the cycle is 1100 K. On the basis of cold air-standard analysis, using ๐๐ฃ =
0.718๐๐ฝ/ ๐๐โ๐พ and ๐๐ = 1.005๐๐ฝ/ ๐๐โ๐พ
, determine theย
(a) the temperature at the end of the compression stroke, in K
(b)peak pressure, in kPa
(c) Heat Addition, kJ/kg
(d) net work of the cycle, kJ/kg
(e)thermal Efficiency.
Solution:
The PV diagram for the Otto cycle is given as
Process 1 -2 is the adiabatic compression.
Process 2 - 3 is the Heat addition at constant volume
Process 3 - 4 is the adiabatic expansion.
Process 4 - 1 is the Heat rejection at constant volume.
At the start of the compression, we are given the pressure and temperature
which is equal to P1 = 95 kPa and T1 = 300K.
We are already given the compression ratio = 9.5
"So, \\frac{V_1}{V_2} = \\frac{V_3}{V_4} = 9.5"
V1 = V3 and V2 = V4 because process 2-3 and 4-1 are at constant volume.
Step 1: To find the temperature at the end of the compression stroke
We can use the formula
"\\frac{T_2}{T_1} = (\\frac{V_1}{V_2} )^{(k-1)}"
where 'k' is the specific heat ratio of the gas. "k=\\frac{C_p}{C_v} = \\frac{1.005kJ\/kg.K}{0.718kJ\/kg.K} = 1.4"
substitute T1 = 300K, V1/V2 = 9.5 and k = 1.4 in the formula we have
"\\frac{T_2}{300K} = (9.5 )^{(1.4-1)}"
"\\frac{T_2}{300K} = (9.5 )^{(0.4)} = 2.4609;"
T2 = 2.4609 * 300K = 738.3 K.
Step 2: To find P2.
P1 = 95kPa, T1 = 300K , T2 = 738.3K V1/V2 = 9.5
"\\frac{P_1V_1}{T_1}=\\frac{P_2V_2}{T_2}"
"\\frac{P_1T_2V_1}{T_1V_2}=P_2"
"\\frac{95kPa*738.3K*9.5}{300K}=P_2"
P2 = 2221kPa
Step 3: To find peak pressure in 'kPa'
In the diagram, we can see that the peak pressure is P3. We have to find out this peak pressure.
Process 2-3 is the Heat addition at constant volume.
In this process addition of heat is taking place at constant volume. This increases the temperature, so the temperature will reach maximum in this step.
Hence T3 = maximum temperature = 1100K.
We can use the formula, "\\frac{P_3V_3}{T_3}=\\frac{P_2V_2}{T_2}" and find the Peak pressure.
volume is constant in this step, so V3 = V2, we can cancel out V3 and V2 from both the side.
"\\frac{P_3}{T_3}=\\frac{P_2}{T_2}"
substitute P2 = 2221kPa, T3 = 1100K, T2= 738.3K and find maximum pressure P3.
"\\frac{P_3}{1100K}=\\frac{2221kPa}{738.3K}"
"P_3=\\frac{2221kPa*1100K}{738.3K}"
P3 = 3309 kPa.
which in 2 significant figures is 3300 kPa.
Hence the peak pressure will be 3300 kPa.
Step 4: To find the heat added in kJ/kg.
Heat is added in the process 2 - 3. This process is taking place at constant volume.
We can use the formula
Q added = Cv * ( T3- T2) = 0.718kJ/kg.K * (1100K-738.3K)
= 0.718 kJ/kg.K* 361.7K = 259.7kJ/kg.
= 260 kJ/kg.
Step 5: To find net work done of the cycle.
The difference between the Qadded and Q rejected will given us the amount of work done by the cycle.
I process 4-1 heat is rejected by the cycle. This process is also taking place at constant volume. But before that you will need T4. We can use the same formula which we used in
Step 1 and find the T4.
"\\frac{T_4}{1100K} = (9.5)^{-(1.4-1)} = 9.5^{-0.4} = 0.4064"
T3 = 1100K * 0.4064 = 447 K
Q rejected = Cv * ( T1 - T4 ) = 0.718 kJ/kg.K * ( 300K - 447K)
= 104.08 kJ/kg
Work done = Q added - Q rejected = 260kJ/kg - 104.08 kJ/kg
= 155.9 kilojoules.
Step 6 : To find Thermal efficiency ,
ฮท = work done/ Q added = 155.9kJ / 260kJ = 0.5997 = 0.6
Hence the thermal efficiency of the given cycle will be 0.6 or 60.0 %
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