Given a gas under #600*"mm Hg"# pressure, and at #303.15*K# temperature, that occupies a volume of #2.02*L#, what volume will it occupy at #273.15*K# temperature, under #750*"mm Hg"# pressure?

Answer 1

Well, the current definition of #"STP"# is.... a temperature of #273.15*K# and a pressure of exactly #10^5*Pa# #(100*kPa, 1*"bar")#.

And #1*"bar"-=(1*"bar")/(1.01325*atm*"bar"^-1)=0.987*atm#
I do all this rigmarole BECAUSE I know that #1*atm# will support a column of mercury that is #760*mm# high...........
And hence in terms of the length of a mercury column, #1*"bar"-=760*mm*Hg*atm^-1xx0.987*atm=750.0*mm*Hg#
#(P_1V_1)/T_1=(P_2V_2)/T_2#
We want #V_2=(P_1V_1)/T_1xxT_2/P_2#
#(600.0*mm*Hgxx2.02*L)/(303.15*K)xx(273.15*K)/(750*mm*Hg)#
#~=1.5*L#
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Answer 2

To solve this problem, you can use the combined gas law, which states:

[ P_1 \times V_1 \div T_1 = P_2 \times V_2 \div T_2 ]

Where:

  • ( P_1 ) and ( P_2 ) are the initial and final pressures, respectively.
  • ( V_1 ) and ( V_2 ) are the initial and final volumes, respectively.
  • ( T_1 ) and ( T_2 ) are the initial and final temperatures, respectively.

Given:

  • ( P_1 = 600 , \text{mm Hg} )
  • ( T_1 = 303.15 , \text{K} )
  • ( V_1 = 2.02 , \text{L} )
  • ( P_2 = 750 , \text{mm Hg} )
  • ( T_2 = 273.15 , \text{K} )

We need to find ( V_2 ), the final volume.

First, we rearrange the equation:

[ V_2 = \frac{{P_1 \times V_1 \times T_2}}{{P_2 \times T_1}} ]

Then, we plug in the given values and solve for ( V_2 ):

[ V_2 = \frac{{600 , \text{mm Hg} \times 2.02 , \text{L} \times 273.15 , \text{K}}}{{750 , \text{mm Hg} \times 303.15 , \text{K}}} ]

[ V_2 = \frac{{330453.39}}{{227372.25}} ]

[ V_2 \approx 1.45 , \text{L} ]

Therefore, the gas will occupy approximately 1.45 liters at 273.15 K temperature under 750 mm Hg pressure.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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