Thermodynamics

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New answer posted•a year ago
S
a year ago

Δ Q = Δ U + Δ W

⇒ Q = Δ U + Q 5 ⇒ Δ U = 4 Q 5 = n C v Δ T ⇒ 4 Q 5 = 5 R 2 Δ T ⇒ Δ T = 8 Q 2 5 R

Q = n c Δ T = 1 × C × 8 0 2 5 R ⇒ C = 2 5 R 8 ⇒ x = 2 5

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

U = 3PV + 4

⇒ n   C v T = 3 P V + 4

⇒ n × f R T 2 = 3 P V + 4

⇒ f = 6 + 8 P V

⇒ f > 6 ⇒ p o l y     a t o m i c

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

P = kV3 Þ PV-3 = k Þ Polytropic Process with index m = -3

W = n R ( T 2 − T 1 ) 1 − m = n R ( 3 0 0 − 1 0 0 ) 1 − ( − 3 ) = 5 0 n R .

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New answer posted•a year ago
S
a year ago

At constant pressure,

d U = n C V d T = n . 5 2 R     d T

d Q = n C P d T = n . 7 2 R     d T

dW = nRdT

dU : dQ : dW = 5 : 7 : 2

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New answer posted•a year ago
S
a year ago

Since process is isochoric

So    Δ U = n C v Δ T


Δ U = n ( 5 2 R ) Δ T − − ( i ) [ C V = 5 2 R ]      

And external work


Δ W = n R Δ T − − ( i i )    

5 2 = x 1 0 ⇒ x = 2 5 . 0 0                

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New answer posted•a year ago
S
a year ago

from newtan’s law of cooling :

d T d t = − k ( T − T 0 )

Using average value :

7 5 − 6 5 5 = − k [ ( 7 5 + 6 5 ) 2 2 − 2 5 ]

( 6 5 − T ) 5 = − k [ ( 6 5 + T ) 2 − 2 5 ]

⇒ 1 0 6 5 − T = 4 5 6 5 + T 2 − 2 5

⇒ T = 5 7 ° C

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New answer posted•a year ago
S
a year ago

Total energy of monoatomic gas at equilibrium

= 3 2 K B T

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New answer posted•a year ago
S
a year ago

From   Δ H = Δ G + T Δ S ∴ Δ S = Δ H − Δ G T

∴ Δ S = [ 5 1 . 4 − ( − 4 9 . 4 ) 3 0 0 ] × 1 0 0 0 J K − 1 m o l − 1 = 3 3 6 J K − 1 m o l − 1

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