The gas inside of a container exerts #25 Pa# of pressure and is at a temperature of #450 ^o K#. If the temperature of the gas changes to #150 ^oC# with no change in the container's volume, what is the new pressure of the gas?
The pressure is
We use Gay Lussac's Law
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To find the new pressure of the gas, we 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 ideal gas constant, and (T) is temperature in Kelvin.
Since the volume of the container remains constant, we can simplify the equation to (\frac{P_1}{T_1} = \frac{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, respectively.
Given: (P_1 = 25 , \text{Pa}) (T_1 = 450 , \text{K}) (T_2 = 150 , ^\circ C = 150 + 273 = 423 , \text{K})
Now, we can rearrange the equation to solve for (P_2): (P_2 = \frac{P_1 \times T_2}{T_1})
Substituting the given values: (P_2 = \frac{25 \times 423}{450})
(P_2 ≈ 23.33 , \text{Pa})
So, the new pressure of the gas is approximately (23.33 , \text{Pa}).
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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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