Pump compresses air into a tank

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Homework Help Overview

The problem involves a cylindrical pump that compresses air into a tank, with specific parameters including length, atmospheric pressure, and manometric pressure. The context is related to thermodynamics, particularly focusing on adiabatic processes and the behavior of gases under pressure.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to apply the adiabatic process equation to find the distance at which air enters the tank, while also considering the ideal gas law as an alternative approach. Some participants question the use of natural logarithms and the assumptions made regarding pressures.

Discussion Status

Participants are actively discussing the calculations involved, with some providing corrections and alternative methods. There is no explicit consensus on the best approach, but guidance has been offered regarding the use of logarithmic transformations and assumptions about pressure.

Contextual Notes

There are indications of confusion regarding the definitions of pressures used in the calculations, as well as the implications of assuming an adiabatic process. The original poster notes the challenge of having two unknowns when not assuming adiabatic conditions.

Karol
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Homework Statement


A cylindrical pump of length 25[cm] pumps air in atmoshpheric pressure ant temp 270C into a big tank. the manometric pressure in the tank is 4[atm]. at which distance will the air start entering the tank.

Homework Equations


In adiabatic process: ##P_1V_1^\gamma=P_2V_2^\gamma##
γ for air=1.4

The Attempt at a Solution


I assume an adiabatic process. i think that manometric pressure is gauge pressure:
$$P_1V_1^\gamma=P_2V_2^\gamma\rightarrow V_2=\sqrt[\gamma]{\frac{P_1}{P_2}V^{\gamma}}$$
$$\rightarrow \ln V_2=\ln\left(\frac{P_1}{P_2}V_1^{\gamma}\right)^{\frac{1}{\gamma}}=\frac{1}{\gamma}\ln\left(\frac{P_1}{P_2}V_1^{\gamma}\right)$$
$$\ln V_2=\frac{1}{\gamma}\left[\ln\left(P_1V_1^{\gamma}\right)-\ln P_2\right]=\frac{1}{\gamma}\left[\ln P_1+\gamma\ln V_1-\ln P_2\right]$$
The volume is area A times length x. for our data:
$$\ln V_2=\ln A+\ln x=\frac{1}{1.4}\left[\ln 0+1.4\ln (A\cdot 25)-\ln 5\right]=\frac{1}{1.4}\left[1.4(\ln A+\ln 25)-\ln 5\right]$$
$$\ln A+\ln x=\ln A+\ln 25-\ln 5\rightarrow \ln x=\ln\left(\frac{25}{5}\right)=\ln 5\rightarrow x=5[cm]$$
It should be 7.9[cm] before the end of the cylinder.
If i don't assume adiabatic process and only use ##PV=nRT## i have 2 unknowns: the distance and the final temperature.
 
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You forgot to divide ln(P2) by 1.4.
Also, P1 = 1, so you shouldn't have ln(0) in the equation.
Also, it was not necessary to work this problem in terms of natural logs.

Chet
 
$$\ln A+\ln x=\ln A+\ln 25-\frac{\ln 5}{1.4}\rightarrow x=7.9[cm]$$
Which other way besides natural logs?
 
Karol said:
$$\ln A+\ln x=\ln A+\ln 25-\frac{\ln 5}{1.4}\rightarrow x=7.9[cm]$$
Which other way besides natural logs?
\frac{V_2}{V_1}=\left(\frac{P_1}{P_2}\right)^{1/\gamma}
\frac{x}{25}=0.2^{(1/\gamma)}
Chet
 
Thanks Chet
 

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