A sample of an gas has a volume of 2.25 L at 286 K and 1.13 atm. What is the pressure when the volume is 1.89 L and temperature is 302 K?
The combined gas law holds that
Why are the units of pressure in the RHS expression clearly as required?
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To solve for the pressure when the volume is 1.89 L and the temperature is 302 K, we can use the combined gas law equation:
(P_1V_1/T_1 = P_2V_2/T_2)
Given: (V_1 = 2.25 , \text{L}) (T_1 = 286 , \text{K}) (P_1 = 1.13 , \text{atm}) (V_2 = 1.89 , \text{L}) (T_2 = 302 , \text{K})
Substituting the values into the equation:
(1.13 , \text{atm} \times 2.25 , \text{L} / 286 , \text{K} = P_2 \times 1.89 , \text{L} / 302 , \text{K})
Solving for (P_2):
(P_2 = (1.13 , \text{atm} \times 2.25 , \text{L} \times 302 , \text{K}) / (286 , \text{K} \times 1.89 , \text{L}))
(P_2 ≈ 1.55 , \text{atm})
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To solve this problem, we can use the combined gas law, which states:
[ \frac{P_1 \cdot V_1}{T_1} = \frac{P_2 \cdot V_2}{T_2} ]
Where:
- ( P_1 ) and ( P_2 ) are the initial and final pressures, respectively.
- ( V_1 ) and ( V_2 ) are the initial and final volumes, respectively.
- ( T_1 ) and ( T_2 ) are the initial and final temperatures, respectively.
Given:
- ( V_1 = 2.25 , \text{L} )
- ( T_1 = 286 , \text{K} )
- ( P_1 = 1.13 , \text{atm} )
- ( V_2 = 1.89 , \text{L} )
- ( T_2 = 302 , \text{K} )
We can plug these values into the combined gas law equation to find ( P_2 ):
[ \frac{(1.13 , \text{atm}) \cdot (2.25 , \text{L})}{286 , \text{K}} = \frac{P_2 \cdot (1.89 , \text{L})}{302 , \text{K}} ]
Solving for ( P_2 ):
[ P_2 = \frac{(1.13 , \text{atm}) \cdot (2.25 , \text{L}) \cdot (302 , \text{K})}{(286 , \text{K}) \cdot (1.89 , \text{L})} ]
[ P_2 \approx \frac{(2.5425 , \text{atm} \cdot \text{L} \cdot \text{K})}{540.74 , \text{L} \cdot \text{K}} ]
[ P_2 \approx 0.0047 , \text{atm} ]
So, the pressure when the volume is ( 1.89 , \text{L} ) and the temperature is ( 302 , \text{K} ) is approximately ( 0.0047 , \text{atm} ).
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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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