The gas inside of a container exerts #27 Pa# of pressure and is at a temperature of #180 ^o K#. If the pressure in the container changes to #40 Pa# with no change in the container's volume, what is the new temperature of the gas?
Approximately
We can apply Gay-Lussac's law, which states that at a constant number of moles and volume, to
or
Thus, by entering our supplied values into the formula, we can obtain,
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Use the ideal gas law: (P_1/T_1 = P_2/T_2)
(T_2 = (P_2/P_1) \times T_1)
(T_2 = (40/27) \times 180)
(T_2 ≈ 266.67 , K)
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Using the ideal gas law (PV = nRT), where (P) is pressure, (V) is volume, (n) is the number of moles, (R) is the gas constant, and (T) is temperature in Kelvin, we can solve for the new temperature ((T_2)):
[P_1V = nRT_1] [P_2V = nRT_2]
Since the volume ((V)) and the number of moles ((n)) remain constant:
[P_1T_1 = P_2T_2]
Substituting the given values:
[27 \times 180 = 40 \times T_2]
[T_2 = \frac{27 \times 180}{40}]
[T_2 = \frac{4860}{40}]
[T_2 = 121.5 , K]
So, the new temperature of the gas is (121.5 , K).
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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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