Science, asked by Arabinda2K00, 9 months ago

air at 1.02 bar 22 degree certificate initially occupies a cylinder volume of .015m³ is compressed isentropically by the piston to a pressure of 0.8 bar. Determine the final temperature, final volume and work done ?​

Answers

Answered by jigarmansuri786
0

Answer:

Explanation:

2.751 j

Initial pressure,         p_{1} = 1.02p  

1

​  

=1.02 bar

 

Initial temperature,          T_{1} = 22 + 273 = 295T  

1

​  

=22+273=295 K

 

Initial volume,       V_{1} = 0.015 m^{3}V  

1

​  

=0.015m  

3

 

 

Final pressure,        p_{2} = 6.8p  

2

​  

=6.8 bar

 

Law of compression :      pv^{\gamma } = Cpv  

γ

=C

 

(i) Final temperature :

 

Using the relation,

 

\frac{T_{2}}{T_{1}}\left ( \frac{P_{2}}{P_{1}} \right )^{\frac{\gamma -1}{\gamma }}  

T  

1

​  

 

T  

2

​  

 

​  

(  

P  

1

​  

 

P  

2

​  

 

​  

)  

γ

γ−1

​  

 

 

 

\frac{T_{2}}{295}=\left ( \frac{6.8}{1.02} \right )^{\frac{1.4-1}{1.4}}  

295

T  

2

​  

 

​  

=(  

1.02

6.8

​  

)  

1.4

1.4−1

​  

 

          [\because γ for \, air = 1.4][∵γforair=1.4]

 

\therefore∴          T_{2}295\left ( \frac{6.8}{1.02} \right )\frac{1.4-1}{1.4}= 507.24T  

2

​  

295(  

1.02

6.8

​  

)  

1.4

1.4−1

​  

=507.24 K

 

i.e.   Final temperature = 507.24 – 273 = 234.24°C507.24–273=234.24°C .

 

(ii) Final volume :

 

Using the relation,

 

p_{1}V_{1}^{\gamma }=P_{2}V_{2}^{\gamma }p  

1

​  

V  

1

γ

​  

=P  

2

​  

V  

2

γ

​  

 

 

\frac{P_{1}}{P_{2}}=\left ( \frac{V_{2}}{V_{1}} \right )^{\gamma }  

P  

2

​  

 

P  

1

​  

 

​  

=(  

V  

1

​  

 

V  

2

​  

 

​  

)  

γ

   or   \frac{V_{2}}{V_{1}}=\left ( \frac{P_{1}}{P_{2}} \right )^{\frac{1}{\gamma }}  

V  

1

​  

 

V  

2

​  

 

​  

=(  

P  

2

​  

 

P  

1

​  

 

​  

)  

γ

1

​  

 

 

 

\therefore∴         V_{2}=V_{1}\times \left ( \frac{P_{1}}{P_{2}} \right )^{\frac{1}{\gamma }}=0.015\times \left ( \frac{1.02}{6.8} \right )^{\frac{1}{1.4}}=0.00387 m^{3} V  

2

​  

=V  

1

​  

×(  

P  

2

​  

 

P  

1

​  

 

​  

)  

γ

1

​  

 

=0.015×(  

6.8

1.02

​  

)  

1.4

1

​  

 

=0.00387m  

3

 

 

i.e.,    Final volume =  0.00387 m^{3} 0.00387m  

3

 .

 

(iii) Wond done :

 

Now,   work done on the air,

 

W=\frac{mR\left ( T_{1}-T_{2} \right )}{\left ( \gamma -1 \right )}W=  

(γ−1)

mR(T  

1

​  

−T  

2

​  

)

​  

       …(i)

 

where m is the mass of air and is found by the following relation

 

pV = mRT

 

\therefore∴        m=\frac{p_{1}V_{1}}{RT_{1}}=\frac{1.02\times 10^{5}\times 0.015}{0.287\times 10^{3}\times 295}m=  

RT  

1

​  

 

p  

1

​  

V  

1

​  

 

​  

=  

0.287×10  

3

×295

1.02×10  

5

×0.015

​  

          \left [ \because R for \, air = 0.287 ×10^{3} \right ][∵Rforair=0.287×10  

3

]

 

= 0.01807 kg

 

\therefore∴        W=\frac{0.01807\times 0.287\times 10^{3}\left ( 295-507.24 \right )}{\left ( 1.4-1 \right )}=-2751J or – 2.751W=  

(1.4−1)

0.01807×0.287×10  

3

(295−507.24)

​  

=−2751Jor–2.751 kJ

 

i.e.,   Work done = 2.751 kJ.

 

(–ve sign indicates that work is done on the air).

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