A gas occupies 1676 mL at -85.1 °C and 225 mmHg. What will its temperature be when its volume is 838 mL at 3.5 atm?

Answer 1

The new temperature would be 839 °C.

To solve this problem, we can use the Combined Gas Laws:

#color(blue)(bar(ul(|color(white)(a/a)(p_1V_1)/T_1 = (p_2V_2)/T_2color(white)(a/a)|)))" "#
We can solve this equation for #T_2#.
#T_2 = T_1 × p_2/p_1 × V_2/V_1#

In this problem,

#p_1 = 225 color(red)(cancel(color(black)("mmHg"))) × "1 atm"/(760 color(red)(cancel(color(black)("mmHg")))) = "0.2960 atm"; p_2 = "3.5 atm"#
#V_1 = "1676 mL";color(white)(mmmmmmmmmmmmmmmll) V_2 = "838 mL"#
#T_1 = "(-85.1 + 273.15) K = 188.05 K";color(white)(mmmmm) T_2 = ?#
∴ #T_2 = "188.05 K" × (3.5 color(red)(cancel(color(black)("atm"))))/(0.2960 color(red)(cancel(color(black)("atm")))) × (838 color(red)(cancel(color(black)("mL"))))/(1676 color(red)(cancel(color(black)("mL")))) = "1112 K" = "839 °C"#

The new temperature is 839 °C.

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Answer 2

To solve this, we can use the combined gas law formula:

[ \frac{P_1 \times V_1}{T_1} = \frac{P_2 \times V_2}{T_2} ]

Where:

  • ( P_1 = 225 , \text{mmHg} )
  • ( V_1 = 1676 , \text{mL} )
  • ( T_1 = -85.1 , \text{°C} + 273.15 , \text{K} ) (Convert -85.1 °C to Kelvin)
  • ( P_2 = 3.5 , \text{atm} )
  • ( V_2 = 838 , \text{mL} )
  • ( T_2 ) is what we're solving for.

First, let's convert -85.1 °C to Kelvin: [ T_1 = -85.1 , \text{°C} + 273.15 , \text{K} = 188.05 , \text{K} ]

Now we can plug these values into the formula: [ \frac{225 , \text{mmHg} \times 1676 , \text{mL}}{188.05 , \text{K}} = \frac{3.5 , \text{atm} \times 838 , \text{mL}}{T_2} ]

Now we can solve for ( T_2 ): [ T_2 = \frac{3.5 , \text{atm} \times 838 , \text{mL} \times 188.05 , \text{K}}{225 , \text{mmHg} \times 1676 , \text{mL}} ] [ T_2 = \frac{3.5 \times 838 \times 188.05}{225 \times 1676} ] [ T_2 = \frac{560227.3}{377400} ] [ T_2 = 1.484 , \text{K} ]

So, the temperature will be approximately 1.484 K.

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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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