A gas has a density of #3.18*g*L^-1# at a temperature of #347*K#, and a pressure of #1.2*atm#. What is its molecular mass?

Answer 1

We use the Ideal Gas equation to get #"molecular mass"=75.5*g*mol^-1#

We assume ideality, and so #PV=nRT#, and thus,
#PV=("mass"/"molar mass")RT# because #n="mass"/"molar mass"#
On rearrangement, #"molar mass"="mass"/Vxx(RT)/P#
But #"mass"/V=rho, "density"#, and thus...........
#"molar mass"=(rhoRT)/P=#
#(3.18*g*L^-1xx0.0821*(L*atm)/(K*mol)xx347*K)/(1.2*atm)#

I am not immune to errors, so let's just cancel out the units to make sure we got this right.

#"Molar mass"=(3.18*g*cancel(L^-1)xx0.0821*cancel(L*atm)/(cancelK*mol)xx347*cancelK)/(1.2*cancel"atm")#

And this provides, I believe, an answer of...

#75.5*g*mol^-1#. Because we have got consistent units, I think our order of operations is correct.
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Answer 2

To find the molecular mass of the gas, you can use the ideal gas law equation:

[ PV = nRT ]

Rearrange the equation to solve for the number of moles (( n )):

[ n = \frac{PV}{RT} ]

Then, use the formula for density to find the number of moles per liter (( n/V )):

[ \frac{n}{V} = \frac{\text{density}}{molar\ volume} ]

Finally, rearrange the equation to solve for the molecular mass (( M )):

[ M = \frac{molar\ mass}{molar\ volume} = \frac{molar\ mass \times RT}{PV} ]

Plug in the given values:

[ M = \frac{molar\ mass \times 0.0821 \times 347}{1.2} ]

Given that the density is ( 3.18 , g/L ), and the molar mass is in grams per mole, we can directly use the density as the molar mass:

[ M = \frac{3.18 \times 0.0821 \times 347}{1.2} ]

[ M = 74.45 , g/mol ]

So, the molecular mass of the gas is approximately ( 74.45 , g/mol ).

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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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