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Mars2501 [29]
3 years ago
15

Air enters a compressor operating at steady state at a pressure of 1 ????????????, a temperature of 290 K, and a velocity of 6 m

???? through an inlet with an area of 0.1 m2 . At the exit, the pressure is 7 ????????????, the temperature is 450 K and the velocity is 2 m ???? . Heat transfer from the compressor to its surroundings occurs at a rate of 180 ???????? m???????? . Employing the ideal gas model, calculate the power input to the compressor in ????W.
Engineering
1 answer:
zmey [24]3 years ago
4 0

Answer: -119.56Kw.

Explanation:

Bringing out the parameters from the equation;

Inlet pressure P1 1bar = 10N/m

Outlet pressure P2 7bar = 70N/m

T1 is 290K, T2 is 450K

Velocity V1 is 6m/s, V2 is 2m/s

Heat transfer rate is 180kj/min. which can be written as 180kj/60secs.

Area A is 0.1m³.

From the steady state energy equation

∆H+g(z2-z1)+1/2(V²2-V²1)=Q/m-W/m

Solving for W with g(z2-z1)=0, we have

∆H+0+1/2(V²2-V²1)=Q/m-W/m

W=Q+m[∆H+(V²2-V²1/2)] ..........eq. 1

m is the mass flow rate given as

A.V/v,

Where W is the power, V is the velocity, and v is the specific volume

A is Area.

But the specific volume is derived from the ideal gas law;

v = (R/M) × T/P1, where R is universal gas constant given as 8314N.m

M is the molecular mass of air given as 28.97kg.k.

STEP 1: Find the specific volume from above formula:

Specific volume, v = [(8314N.m/28.97kg.k) × 290K]/ 10N/m² = 0.8324kg/m³

STEP 2: Find mass flow rate, m = A.V/v = 0.1m³ × 6m/s / 0.8324kg/m³

m = 0.7209kg/s

STEP 3: Find the specific enthalpy from air property table as

@ T1 of 290k and P1 of 0.1Mpa, specific enthalpy is 290.6kj,/kg

@T2 of 450k and P2 of 0.7Mpa, specific enthalpy is 452.3kj/kg.

Therefore, ∆H = H2 - H1 = 290.6kj/kg - 452.3kj/kg = -161.7kj/kg.

STEP 4: Calculate change in K.E

1/2(V²2-V²1) = 6²-2² /2 = 16J/kg or 0.016Kj/kg..

STEP 5: Calculate power in KW using eq.1.

W = (180kj/60secs) + [(0.7209kj/s(-161.7-0.016)kj/kg]

W = 3kj/secs - 116.557kj.s

W = -119.56KW.

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3 years ago
The steady-state data listed below are claimed for a power cycle operating between hot and cold reservoirs at 1200K and 400K, re
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Answer:

a) W_cycle = 200 KW , n_th = 33.33 %  , Irreversible

b) W_cycle = 600 KW , n_th = 100 %     , Impossible

c) W_cycle = 400 KW , n_th = 66.67 %  , Reversible

Explanation:

Given:

- The temperatures for hot and cold reservoirs are as follows:

  TL = 400 K

  TH = 1200 K

Find:

For each case W_cycle , n_th ( Thermal Efficiency ) :

(a) QH = 600 kW, QC = 400 kW

(b) QH = 600 kW, QC = 0 kW

(c) QH = 600 kW, QC = 200kW

- Determine whether the cycle operates reversibly, operates irreversibly, or is impossible.

Solution:

- The work done by the cycle is given by first law of thermodynamics:

                                 W_cycle = QH - QC

- For categorization of cycle is given by second law of thermodynamics which states that:

                                 n_th < n_max     ...... irreversible

                                 n_th = n_max     ...... reversible

                                 n_th > n_max     ...... impossible

- Where n_max is the maximum efficiency that could be achieved by a cycle with Hot and cold reservoirs as follows:

                                n_max = 1 - TL / TH = 1 - 400/1200 = 66.67 %

And,                         n_th = W_cycle / QH

a) QH = 600 kW, QC = 400 kW

   - The work done by cycle according to First Law is:

                                W_cycle = 600 - 400 = 200 KW

   - The thermal efficiency of the cycle is given by n_th:

                                n_th = W_cycle / QH

                                n_th = 200 / 600 = 33.33 %

   - The type of process according to second Law of thermodynamics:

               n_th = 33.333 %                n_max = 66.67 %

                                       n_th < n_max  

      Hence,                Irreversible Process  

b) QH = 600 kW, QC = 0 kW

   - The work done by cycle according to First Law is:

                                W_cycle = 600 - 0 = 600 KW

   - The thermal efficiency of the cycle is given by n_th:

                                n_th = W_cycle / QH

                                n_th = 600 / 600 = 100 %

   - The type of process according to second Law of thermodynamics:

                 n_th = 100 %                 n_max = 66.67 %

                                     n_th > n_max  

      Hence,               Impossible Process              

c) QH = 600 kW, QC = 200 kW

   - The work done by cycle according to First Law is:

                                W_cycle = 600 - 200 = 400 KW

   - The thermal efficiency of the cycle is given by n_th:

                                n_th = W_cycle / QH

                                n_th = 400 / 600 = 66.67 %

   - The type of process according to second Law of thermodynamics:

               n_th = 66.67 %                 n_max = 66.67 %

                                     n_th = n_max  

      Hence,                Reversible Process

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Explanation:

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Lehr is the long open or closed insulated space for glass manufacturing. Lehr must be large enough to keep the cooling of glass uniform. The function of Lehr is the same as an annealing process in metallurgy.  

Step2

Lehr decrease the cooling and temperature variation in glass production. Uneven temperature creates the internal stress in the glass. Lehr reduces the internal stress in the glass product.  So, the main purpose of the Lehr is to reduce the internal stress and keep the cooling uniform.

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