The gas inside of a container exerts #"24 Pa"# of pressure and is at a temperature of #"320 K"#. If the pressure in the container changes to #"32 Pa"# with no change in the container's volume, what is the new temperature of the gas?

Answer 1

The final temperature is 430 K.

This is an example of Guy-Lussac's law, which states that as long as volume is constant, the pressure and temperature of a gas are directly proportional. This means that if the pressure goes up, so does the temperature and vice-versa. The equation for Gay-Lussac's law is #P_1/T_1=P_2/T_2#, where #P_1# is the initial temperature, #T_1# is the initial temperature, #P_2# is the final temperature, and #T_2# is the final temperature.
Given #P_1="24 Pa"# #T_1="320 K"# #P_2="32 Pa"#
Unknown #T_2#
Solution Rearrange the equation to isolate #T_2#. Substitute the given values into the equation and solve.
#P_1/T_1=P_2/T_2#
#T_2=(P_2T_1)/P_1#
#T_2=(32cancel"Pa"xx320"K")/(24cancel"Pa")="430 K"# rounded to two significant figures
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Answer 2

You can use the ideal gas law, ( PV = nRT ), where ( P ) is pressure, ( V ) is volume, ( n ) is the number of moles of gas, ( R ) is the gas constant, and ( T ) is temperature. Since the volume remains constant, we can simplify the equation to ( P_1/T_1 = P_2/T_2 ) where ( P_1 ) and ( T_1 ) are the initial pressure and temperature, and ( P_2 ) and ( T_2 ) are the final pressure and temperature.

Given that ( P_1 = 24 , \text{Pa} ), ( T_1 = 320 , \text{K} ), and ( P_2 = 32 , \text{Pa} ), we can rearrange the equation to solve for ( T_2 ):

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

[ T_2 = \frac{{32 , \text{Pa} \times 320 , \text{K}}}{{24 , \text{Pa}}} ]

[ T_2 = 426.67 , \text{K} ]

So, the new temperature of the gas is ( 426.67 , \text{K} ).

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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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