Air in a piston–cylinder assembly, initially at 3 bar, 142 K, and a volume of 2 m3. The air undergoes a process to a state where the pressure is 1.5 bar, during which the pressure–volume relationship is pV = constant. Assuming ideal gas behavior for the air, determine: the mass of the air, in kg and the work and heat transfer, each in KJ.

Respuesta :

Answer:

mass of the air = 14.62kg

Workdone = 415.88 kJ

Heat transfer = 415.88 kJ

Explanation:

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Ver imagen temdan2001
Ver imagen temdan2001

Answer:

(a) 14.72 kg

(b) 414 kJ

(c) 414 kJ

Explanation:

(a) To get the mass of the air, the ideal gas equation will be used and is given as follows;

PV = mRT Ā  Ā  Ā  Ā  Ā  Ā ----------------(i)

Where;

P = pressure of the air = 3 bar = 3 x 10⁵Pa

V = volume of the air = 2m³

m = mass of air

R = specific gas constant of air = 287.05 [tex]\frac{J}{kgK}[/tex]

T = temperature of the air = 142K

Substitute these values into equation (i) as follows;

3 x 10⁵ x 2 = m x 287.05 x 142

6 x 10⁵ = m x 40761.1

600000 = 40761.1m

m = [tex]\frac{600000}{40761.1}[/tex]

m = 14.72kg

Therefore, the mass of the air is 14.72 kg

(b) According to the question, the relationship between the pressure and the volume is given by

PV = k Ā  Ā  Ā  Ā  (where k = constant)

This implies that;

P₁V₁ = Pā‚‚Vā‚‚ = ... = k Ā  Ā  Ā  Ā  Ā  -------------------(ii)

Where;

P₁ = initial pressure of air = 3 bar = 3 x 10⁵Pa

V₁ = initial volume of air = 2m³

Pā‚‚ = final pressure of air = 1.5 bar = 1.5 x 10⁵Pa

Vā‚‚ = final volume of air

Substitute these values into equation (ii) as follows;

3 x 10⁵ x 2 = 1.5 x 10⁵ x Vā‚‚

6 x 10⁵ = 1.5 x 10⁵Vā‚‚

6 = 1.5Vā‚‚

Vā‚‚ = [tex]\frac{6}{1.5}[/tex]

Vā‚‚ = 4m³

Also, from equation (ii)

P₁V₁ = k Ā  Ā  Ā  Ā  Ā  Ā  Ā  --------------(iii)

Substitute the values of P₁ and V₁ into equation (iii) as follows;

3 x 10⁵ x 2 = k

k = 6 x 10⁵ m³Pa

Recall that PV = k

This implies that;

P = [tex]\frac{k}{V}[/tex] Ā  Ā  Ā  Ā  Ā  Ā ------------(iv)

Also, remember, in thermodynamics the work done, W, when a gas expands or compresses in volume is given by the following;

W = [tex]\int\limits^{V_2}_{V_1} {P} \, dV[/tex]

Substitute the value of P in equation (iv) into the above equation as follows;

W = [tex]\int\limits^{V_2}_{V_1} {\frac{k}{V} } \, dV[/tex]

W = [tex]k \int\limits^{V_2}_{V_1} {\frac{1}{V} } \, dV[/tex]

W = [tex]k \int\limits^{V_2}_{V_1} {V^{-1} } \, dV[/tex]

Integrating gives;

W = k ln [V] Ā  Ā  Ā  Ā  Ā  Ā  Ā  Ā -----------------(v)

Putting the values of the integral limits V₁ and Vā‚‚ into equation (v)

W = k ln [Vā‚‚ - V₁]

Substitute the values of k, Vā‚‚ and V₁ into equation above as follows;

W = 6 x 10⁵ ln [4 - 2]

W = 6 x 10⁵ ln [2]

W = 6 x 10⁵ (0.69)

W = 4.14 x 10⁵

W = 414 kJ

Therefore, the work done is 414 kJ

(c) The heat transfer Q, the work done, W, and the change in internal energy, ΔU, in a thermodynamic system are related by the following relation;

Q - W = ΔU                  ----------(vi)

If the values of Pā‚‚, Vā‚‚ are substituted into equation (i) to find the value of Tā‚‚, it will be found that T₁ and Tā‚‚ are the same. i.e T₁ = Tā‚‚ = 142K. Therefore, the change in internal energy, Ī”U = 0.

Equation (vi) the becomes

Q - W = 0

Q = W Ā  Ā  Ā  Ā  Ā  Ā [Substitute the value of W = 414 kJ]

Q = 414 kJ

Therefore, the heat transfer is 414 kJ