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monitta
3 years ago
6

3- A cylinder with 0.4kg of Nitrogen gas at 27ºC keeps under pressure by a frictionless piston. Weight of this piston will incre

ase pressure to 0.35atm more than ambient pressure (which is 1atm) at 27ºC. Therefore, at the beginning Nitrogen is at 1.35atm and at equilibrium with surrounding. Consider these four processes which is happening in order:
A) System is reaching equilibrium after merging into a container of steam.
B) A variable force slowly pushing piston while temperature stay constant at 0ºC and Nitrogen compressed to half of its initial volume. At this point piston will stop by stoppers.
C) Taking the system out from steam container in order to reach equilibrium with surrounding.
D) Now remove stoppers until system reaches completely to equilibrium with surrounding.
Determine Q, W, ΔU, ΔH for the system. (consider Nitrogen as ideal gas)
Engineering
1 answer:
Ivan3 years ago
6 0

<u>Solution and Explanation:</u>

Step 1 Temperature from T =27C to T = 0C constant volume process

Step 2 At 0C volume changes from V1 to V1/2 , isothermally

Step 3 Temperature changes from 0C to 27C , constant volume process

Step 4 Volume changes from V/2 to V1 isothermally at 27C

From the description of the problem it is clear that the problem is a cyclic process , which involves 2 isothermal process at 27C and 0C and two constant volume process at volume coressponding to the volume of ideal gas at the given conditions. since it is a cyclic proess (comes back to the initial state) \triangle \mathrm{H} \& \Delta \mathrm{U} are zero because they are sate functions and in a cyclic process the change in state functions are zero, \Delta \mathrm{H}=\Delta \mathrm{U}=\underline{0}

The first law can be written as\text { Qnet }=\Delta \mathrm{U}+\text { Whet }  with appropriate sign convention , since \Delta \mathrm{U}=0\

Qnet = Wnet    

work is zero for the two constant volume process , contribution to work comes only from isothermal process ,and for ideal gas it is given as \mathrm{W}=\mathrm{nRT} \ln (\mathrm{V} 2 / \mathrm{V} 1)

It is given V 2=V 1 / 2

\mathrm{W}=\mathrm{W} 2+\mathrm{W} 4=\mathrm{nRT} 2 \ln 2-\mathrm{nRT} 4 \ln 2

\mathrm{T} 2=0 \mathrm{C}=273 \mathrm{K} \text { and } \mathrm{T} 4=27 \mathrm{C}=300 \mathrm{K}

n=0.4 * 100 / 28 \text { moles }=14.28

\mathrm{W}=\mathrm{nR} \ln 2 *(273-300)=14.28 * 8.314 * 0.693^{*}-27=-2221.91 \text { joules }, so this amount of work has to be done on the system , since Q= W , Q = -2221.91 Joules of heat is to be transfered from the system.

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Answer:

a) Internal energy

Explanation:

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complete question

A certain amplifier has an open-circuit voltage gain of unity, an input resistance of 1 \mathrm{M} \Omega1MΩ and an output resistance of 100 \Omega100Ω The signal source has an internal voltage of 5 V rms and an internal resistance of 100 \mathrm{k} \Omega.100kΩ. The load resistance is 50 \Omega.50Ω. If the signal source is connected to the amplifier input terminals and the load is connected to the output terminals, find the voltage across the load and the power delivered to the load. Next, consider connecting the load directly across the signal source without the amplifier, and again find the load voltage and power. Compare the results. What do you conclude about the usefulness of a unity-gain amplifier in delivering signal power to a load?

Answer:

3.03 V  0.184 W

2.499 mV  125*10^-9 W

Explanation:

First, apply voltage-divider principle to the input circuit: 1

V_{i}= (R_i/R_i+R_s) *V_s = 10^6/10^6+(0.1*10^6)\\*5

    = 4.545 V

The voltage produced by the voltage-controlled source is:

A_voc*V_i = 4.545 V

We can find voltage across the load, again by using voltage-divider principle:  

V_o = A_voc*V_i*(R_o/R_l+R_o)

      = 4.545*(100/100+50)

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P_L = V_o^2/R_L

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Apply voltage-divider principle to the circuit:  

V_o = (R_o/R_o+R_s)*V_s

       = 50/50+100*10^3*5

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Now we can determine delivered power:  

P_l = V_o^2/R_l

     = 125*10^-9 W

Delivered power to the load is significantly higher in case when we used amplifier, so a unity gain amplifier can be useful in situation when we want to deliver more power to the load. It is the same case with the voltage, no matter that we used amplifier with voltage open-circuit gain of unity.  

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