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IrinaK [193]
4 years ago
13

Dr. Thermo, only has one bottle of neon. However, he needs to run two experiments, each requiring its own bottle. Therefore, he

plans to connect the two bottles together and open the valves on each so that each bottle is partially filled. He wants to know how the enthalpy of the gas will change when he performs this operation. Each bottle has an internal volume of 43.8 L, is completely rigid, and fully insulated. At the start, the full bottle has a pressure of 1.1 MPa, the second bottle is completely evacuated, and both are at room temperature (298 K). After the valves are opened, the two bottles come to equilibrium at 346 kPa. You can assume that neon behaves ideally during this process.
a. Dr. Thermo wants you to derive an equation for H(P.V) and then use that equation to determine the change in enthalpy by integration, showing him all your work.
b. Being a thermo wiz, you know there is another (and easier) way to perform this calculation. Verify your answer to part a using this easier way.
Engineering
1 answer:
nasty-shy [4]4 years ago
7 0

Solution:

The data provided in the question are :

$V_1 = V_2 = 43.8\ L$

             = $ \frac{43.8}{1000}\ m^3$

$ P_1 = 1.1\ MPa$   and   $ P_2 = 0$

Initial pressure of neon = 1.1 MPa

Final Pressure =  346 kPa

Initial temperature of neon = 298 K

$P_1V_1=mRT_1$

$ 1.1 \times 10^6 \times \frac{43.8}{1000} =  m \times \frac{8314}{MM}\times 298$

Molecular mass of neon = 20.1797 g/mole

m = 0.3924 kg

For final temperature:

$P_fV_f=mRT_f$

$V_f = 2 \times \frac{43.8}{1000}$

$ 346 \times 1000 \times 2 \times \frac{43.8}{1000} = m \times \frac{8314}{20.1797} \times T_f$

$ \therefore T_f = 187.48\ K$

a). From first law of thermodynamics :

δQ = δU + δW

Tds = dU + PdV

or dH =  dTs + VdP

As system is insulator,  Tds = 0

$ \Delta H = \left( \frac{P_1V_1-P_2V_2}{\gamma - 1} \right)^{\gamma}$      as  $PV^{\gamma}$  = constant

$P_1V_1^{\gamma}= PV^{\gamma}$

$V= \left( \frac{P_1V_1^{\gamma}}{P} \right)^{\frac{1}{\gamma}}$

Substituting in VdP and integrating, the above equation is obtained.

So, γ = 1.67 (mono atomic neon)

$ \Delta H = 1.67 \times \frac{(1.1 \times 10^6 \times 0.0438 - 346 \times 10^3 \times 2 \times 0.0438)}{1.67-1}$

$ \Delta H = 44942.63\ J$

$ \Delta H = 44.942\ kJ$

b). Easier way is :

$ \Delta H = mC_P\Delta T$

$ \Delta H = 0.3924 \times C_P(T_f-T_1)$

$C_P = \frac{\gamma R}{\gamma-1}$

     $= \frac{1.67 \times 8314}{0.67 \times 20.1797}$

     = 1026.92 J/kg-K

$ \Delta H = 0.3924 \times 1026.92 (187.48-298)$

      $ = -44.585\ kJ$

The negative sign indicates decrease in enthalpy.

The answer by easier way is very near to the value in part (a).

Error (%) =  $ \frac{44.942-44.585}{44.942}  \times 100$

              = 0.015 %   (which is negligible)

Therefore, both the answers are same.

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Answer:

As many variables as we can coherently communicate in 2 dimensions

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A light bulb is switched on and within a few minutes its temperature becomes constant. Is it at equilibrium or steady state.
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Answer:

The temperature attains equilibrium with the surroundings.  

Explanation:

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Thus we conclude that the bulb absorbs as well as dissipates it's absorbed thermal energy. we know that this rate is dependent on the temperature of the bulb thus it the temperature of the bulb does not change we can infer that an equilibrium has been reached in the above 2 processes i.e the rate of energy absorption equals the rate of energy dissipation.

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For a turbulent flow of a fluid in 0.6 m diameter pipe, the velocity 0.15 m from the wall is 2.7 m/s. Estimate the wall shear st
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Kerosene flows through 3/4 standard type K drawn copper tube. The pressure drop measured at two points 50 m apart is 130 kPa. De
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Answer:

Q=4.98\times 10^{-3}\ m^3/s.

Explanation:

Given that

L= 50 m

Pressure drop = 130 KPa

copper tube is 3/4 standard type K drawn tube.

From standard chart ,the dimension of 3/4 standard type K copper tube given as

Outside diameter=22.22 mm

Inside diameter=18.92 mm

Dynamic viscosity for kerosene

\mu =0.00164\ Pa.s

We know that

\Delta P=\dfrac{128\mu QL}{\pi d_i^4}

Where Q is volume flow rate

L is length of tube

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Now by putting the values

\Delta P=\dfrac{128\mu QL}{\pi d_i^4}

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Q=4.98\times 10^{-3}\ m^3/s

So flow rate is Q=4.98\times 10^{-3}\ m^3/s.

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