The gas inside of a container exerts #8 Pa# of pressure and is at a temperature of #220 ^o K#. If the temperature of the gas changes to #20 ^oC# with no change in the container's volume, what is the new pressure of the gas?

Answer 1

The final pressure is #10.66# Pa.

I assume that we are working with a perfect gas. The process is called isochoric (it means that mantains the volume unchanged). Those process follow the law #P/T=#constant.
This mean that if we have an initial pressure and temperature #P_i, T_i# and a final pressure and temperature #P_f, T_f# the law tell us: #P_i/T_i=#constant #P_f/T_f=#constant then #P_i/T_i=P_f/T_f#. In our case we have #P_i=8# Pa #T_i=220# K (you shouldn't use the symbol #\circ# for Kelvin) #T_f=20^\circ# C and we want to know #P_f#.
It is always better to work in the International System then we convert the Celsius in Kelvin adding #273.15#: #T_f=20^\circ# C #=293.15# K.

Before solving the equation of the isochoric process we can notice that the temperature is increasing of 73.15 K from 220 K to 293.15 K. If we warm up a gas we expect that the pressure increase because the particles of the gas move faster. So at the end we should find something bigger than 8 Pa.

We can write our equation for isochoric process #8/220 = P_f/293.15# obtaining #P_f=8/220 293.15=10.66# Pa (that is bigger than 8, as expected from a warmer gas).
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Answer 2

To find the new pressure of the gas when the temperature changes, you can use the ideal gas law equation:

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

Given that the volume and volume remain constant, we can simplify the equation to:

[ P_1 / T_1 = P_2 / T_2 ]

Substituting the given values:

[ 8 , \text{Pa} / 220 , \text{K} = P_2 / (20 + 273.15) , \text{K} ]

Solving for ( P_2 ):

[ P_2 = (8 , \text{Pa} \times (20 + 273.15) , \text{K}) / 220 , \text{K} ]

[ P_2 ≈ 72.36 , \text{Pa} ]

Therefore, the new pressure of the gas is approximately 72.36 Pa.

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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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