A sample of oxygen occupies a volume of 160 dm3 at 91° C. What will be volume of oxygen when the temperature drops to 0.00° C?
The volume of the oxygen will be 120 dm³.
This is an example of Charles' Law.
This makes sense. The final Kelvin temperature was about 25 % lower than the initial temperature. The final volume should be about 25 % (40 dm³) less than the initial volume.
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To find the final volume of oxygen when the temperature drops to 0.00°C, we can use the combined gas law, which relates the initial and final volumes and temperatures of a gas sample:
[ \frac{P_1 \times V_1}{T_1} = \frac{P_2 \times V_2}{T_2} ]
Given:
- Initial volume, (V_1 = 160 , \text{dm}^3)
- Initial temperature, (T_1 = 91 , \text{°C}) (convert to Kelvin by adding 273.15: (T_1 = 91 + 273.15 , \text{K}))
- Final temperature, (T_2 = 0.00 , \text{°C}) (convert to Kelvin: (T_2 = 0.00 + 273.15 , \text{K}))
- We are solving for the final volume, (V_2)
Rearranging the equation to solve for (V_2):
[ V_2 = \frac{T_2 \times P_1 \times V_1}{T_1 \times P_2} ]
Since the pressure (P) is constant in this case, it cancels out:
[ V_2 = \frac{T_2 \times V_1}{T_1} ]
Now, plug in the values to calculate (V_2).
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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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