Pressure of a fluid contained in a steel container

AI Thread Summary
The discussion focuses on calculating the increase in pressure of gasoline in a sealed steel container when the temperature rises by 11 degrees Celsius. Two scenarios are considered: one where the expansion of the container is included and one where it is ignored. The bulk modulus of gasoline is used to determine the pressure increase, with calculations involving the thermal expansion of both the gasoline and the steel container. The final pressure increase, when considering the container's expansion, is calculated to be approximately 1.756 x 10^7 Pa. It is clarified that the absolute pressure would be this increase plus the initial atmospheric pressure.
squelch
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Homework Statement



A steel container is completely filled with gasoline, and then sealed. The temperature is then increased 11 degrees C. If the bulk modulus of gasoline is 1.90 \times {10^9}Pa, find the increase in pressure of the gasoline if:
(a) The expansion of the container is considered.
(b) The expansion of the container is ignored.
(For gasoline, \beta = 9.60 \times {10^{ - 4}}^ \circ {C^{ - 1}})

Homework Equations



\Delta V = {V_0}\beta \Delta T
p = \frac{F}{A} = - Y\alpha \Delta T

The Attempt at a Solution



The volume of the steel container will expand to a final volume:
{V_c} = {V_0}(1 + {\beta _{(steel)}}\Delta T)
Similarly, the volume of the gas expands:
{V_c} = {V_0}(1 + {\beta _{(gasoline)}}\Delta T)

Because we filled the container up to the brim before sealing it, we can assume the initial volumes are equal and that the initial pressure is one atmosphere (how relevant the latter point is I'm not sure). The initial volume isn't given, but I can relate the two ratios:

\frac{{\Delta {V_s}}}{{{\beta _s}}} = \frac{{\Delta {V_g}}}{{{\beta _g}}}

Presumably, the liquid gasoline expands more than the steel canister. I know that pressure = force / area and I know that p = \frac{F}{A} = - Y\alpha \Delta T, but I'm not entirely sure how to apply that latter equation to what I know.
 
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The easiest approach is to treat this as a two-step process. For the case where the container expansion is ignored, first calculate the new volume of the gasoline as if it were completely free to expand (thermal expansion). Then calculate the pressure increase that would be required to squeeze the gasoline back into the container (bulk modulus).

Chet
 
I think my *biggest* problem is that I can't seem to find an expression for the pressure increase required to compress the gasoline back into the container. Obviously this isn't an ideal gas, so I can't use the Ideal Gas Law. I'm not really sure at all what the -Y\alpha \Delta T is trying to say. I just found an expression for the bulk modulus:
B = \frac{{\Delta P}}{{\frac{{\Delta V}}{V}}} = \frac{{\Delta P \cdot V}}{{\Delta V}}
...and I'm trying to proceed from there.
 
squelch said:
I think my *biggest* problem is that I can't seem to find an expression for the pressure increase required to compress the gasoline back into the container. Obviously this isn't an ideal gas, so I can't use the Ideal Gas Law. I'm not really sure at all what the -Y\alpha \Delta T is trying to say. I just found an expression for the bulk modulus:
B = \frac{{\Delta P}}{{\frac{{\Delta V}}{V}}} = \frac{{\Delta P \cdot V}}{{\Delta V}}
...and I'm trying to proceed from there.
I don't know what the Y in your equation stands for, but I'm guessing it is related to the ratio of the coefficient of thermal expansion to the bulk modulus. As far as your approach that you are trying to proceed with, this is the correct way to go.

Chet
 
So I found a procedure and tried to implement it this way:

\begin{array}{l}<br /> \Delta {V_{(container)}} = \Delta {V_{(therm.expan.)}} - \Delta {V_{(stress)}}\\ ⇒<br /> {V_0}{\beta _{(steel)}}\Delta T = {V_0}{\beta _{gasoline}} - \frac{{\Delta P \cdot {V_0}}}{{{B_{gasoline}}}}\\ ⇒<br /> ({\beta _{gasoline}} - {\beta _{steel}})\Delta T{B_{gasoline}} = \Delta P<br /> \end{array}

Plugging in the known constants, and taking the bulk modulus of steel to be 3.6 \times {10^{ - 5}}^o{C^{ - 1}} I get an answer of 1.756 \times {10^7}Pa for the first portion. Does this seem sensible?
 
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squelch said:
So I found a procedure and tried to implement it this way:

\begin{array}{l}<br /> \Delta {V_{(container)}} = \Delta {V_{(therm.expan.)}} - \Delta {V_{(stress)}}\\ ⇒<br /> {V_0}{\beta _{(steel)}}\Delta T = {V_0}{\beta _{gasoline}} - \frac{{\Delta P \cdot {V_0}}}{{{B_{gasoline}}}}\\ ⇒<br /> ({\beta _{gasoline}} - {\beta _{steel}})\Delta T{B_{gasoline}} = \Delta P<br /> \end{array}

Plugging in the known constants, and taking the bulk modulus of steel to be 3.6 \times {10^{ - 5}}^o{C^{ - 1}} I get an answer of 1.756 \times {10^7}Pa for the first portion. Does this seem sensible?
Thats what i also had in mind. b) is the same procedure, with just taking ##\Delta V_{container}=0##
 
Yup, that's the process I'm applying to the latter half. Thanks for the validation.
 
As a last point, I'm actually finding \Delta P, so is it accurate to say I need to add 1 ATM to the pressure?

edit: Upon rereading the question it's clear that this is the pressure reading they want, but I suppose it's worth knowing that the absolute pressure is \Delta P + 1 atm
 
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