A balloon that had a volume of 3.50 L at 25.0 °C is placed in a hot room at 40.0 °C. If the pressure remains constant at 1.00 atm, what is the new volume of the balloon in the hot room?

Answer 1

3.68 liters to three significant numbers.

This issue pertains to Charles Law.

# V_1/T_1 = V_2/T_2#
# V_1 = "3.5 L"#,
# T_1 = 25 + 273 = "298 K"# ,
#V_2 = "unknown L"#,
# T_2 = 40 + 273 = "313 K"#,

thus

# ("3.5 L")/("298 K") = V_2/("313 K")# .

This provides

# ("3.5 L") xx ("313 K")/("298 K") = V_2#.
#=> "3.68 L" = V_2#
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Answer 2

You can use the combined gas law to solve this problem. The combined gas law equation is:

( \frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2} )

Given: (V_1 = 3.50 , \text{L}) (T_1 = 25.0 + 273.15 , \text{K}) (T_2 = 40.0 + 273.15 , \text{K}) (P_1 = P_2 = 1.00 , \text{atm})

Substituting the values into the equation and solving for (V_2):

( \frac{(1.00 , \text{atm})(3.50 , \text{L})}{(25.0 + 273.15) , \text{K}} = \frac{(1.00 , \text{atm})(V_2)}{(40.0 + 273.15) , \text{K}} )

( V_2 = \frac{(1.00 , \text{atm})(3.50 , \text{L})(313.15 , \text{K})}{(298.15 , \text{K})} )

( V_2 ≈ 3.77 , \text{L} )

Therefore, the new volume of the balloon in the hot room is approximately 3.77 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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