A container with a volume of #"16 L"# contains a gas with a temperature of #"180 K"#. If the temperature of the gas changes to #"360 K"# without any change in pressure, what must the container's new volume be?

Answer 1

The final volume will be exactly #"32 L"#.

This is an illustration of Charles' law, which states that the Kelvin temperature is directly proportional to the volume of a given amount of a gas at constant pressure.

You should use the following equation:

#V_1/T_1=V_2/T_2#, where #V# is volume and #T# is temperature in Kelvins.
Known #V_1="16 L"# #T_1="180 K"# #T_2="360 K"#
Unknown #V_2#
Solution Rearrange the equation to isolate #V_2#. Insert the known values and solve.
#V_2=(V_1T_2)/T_1#
#V_2=(16"L"xx360cancel"K")/(180cancel"K")="32 L"#
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Answer 2

Using the ideal gas law equation (PV = nRT), where (P) is pressure, (V) is volume, (n) is the number of moles of gas, (R) is the ideal gas constant, and (T) is temperature in Kelvin, we can rearrange the equation to solve for (V). Since the pressure is constant, we have:

(V_1 / T_1 = V_2 / T_2)

Substituting the given values, we get:

(16 , \text{L} / 180 , \text{K} = V_2 / 360 , \text{K})

Solving for (V_2), we find:

(V_2 = (16 , \text{L} \times 360 , \text{K}) / 180 , \text{K} = 32 , \text{L})

Therefore, the container's new volume must be (32 , \text{L}).

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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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