Problem 39
Question
A balloon filled with \(39.1 \mathrm{moles}\) of helium has a volume of \(876 \mathrm{L}\) at \(0.0^{\circ} \mathrm{C}\) and \(1.00 \mathrm{atm}\) pressure. The temperature of the balloon is increased to \(38.0^{\circ} \mathrm{C}\) as it expands to a volume of \(998 \mathrm{L}\), the pressure remaining constant. Calculate \(q, w,\) and \(\Delta E\) for the helium in the balloon. (The molar heat capacity for helium gas is \(20.8 \mathrm{J} /^{\circ} \mathrm{C} \cdot \mathrm{mol}.\))
Step-by-Step Solution
Verified Answer
The heat (q) absorbed by the helium gas is \(30872.56 \mathrm{J}\), the work (w) done by the gas is \(-12361.7 \mathrm{J}\), and the change in internal energy (ΔE) of the gas is \(18510.86 \mathrm{J}\).
1Step 1: Convert temperatures to Kelvin
Since we will be working with the Ideal Gas Law and temperature changes, it's important to convert the given temperatures from Celsius to Kelvin.
Initial temperature, \(T_1 = 0.0^{\circ} \mathrm{C} = 273.15 \mathrm{K}\)
Final temperature, \(T_2 = 38.0^{\circ} \mathrm{C} = 273.15 + 38.0 = 311.15 \mathrm{K}\)
2Step 2: Calculate the change in volume
To find the work done by the helium gas, we need to find the change in volume.
ΔV = final volume - initial volume
ΔV = \(998 \mathrm{L} - 876 \mathrm{L} = 122 \mathrm{L}\)
3Step 3: Calculate the work done
We know the following equation for work done by a gas when the pressure is constant:
w = -PΔV
In this case, the constant pressure P is given as \(1.00 \mathrm{atm}\). Since we are given heat capacity in J/°C, we should change the pressure unit from atm to Pascal.
\(1 \mathrm{atm} = 101325 \mathrm{Pa}\)
So, w = \(-1.00 \times 101325 \mathrm{Pa} \times 122 \mathrm{L}\)
Convert litres to cubic meters: \(1\mathrm{L} = 0.001\mathrm{m^3}\)
w = \(-101325 \mathrm{Pa} \times 0.122\mathrm{m^3} = -12361.7 \mathrm{J}\)
The work done by the helium gas is -12361.7 J.
4Step 4: Calculate the heat absorbed by the gas
We can use the following equation for the heat absorbed for a constant pressure process:
q = nCΔT
Here, n = 39.1 moles, C = 20.8 J/mol°C, and ΔT = T2 - T1 = 311.15 K - 273.15 K = 38.0 K.
So, q = \(39.1 \mathrm{mol} \times 20.8 \frac{\mathrm{J}}{\mathrm{mol\cdot K}} \times 38.0\mathrm{K} = 30872.56\mathrm{J}\)
The heat absorbed by the helium gas is 30872.56 J.
5Step 5: Calculate the change in internal energy
Now that we have both q and w, we can use the first law of thermodynamics to find ΔE:
ΔE = q + w
ΔE = \(30872.56 \mathrm{J} - 12361.7 \mathrm{J} = 18510.86 \mathrm{J}\)
The change in internal energy of the helium gas is 18510.86 J.
Solution: The heat (q) absorbed by the helium gas is 30872.56 J, the work (w) done by the gas is -12361.7 J, and the change in internal energy (ΔE) of the gas is 18510.86 J.
Key Concepts
Ideal Gas LawMolar Heat CapacityInternal EnergyWork Done by Gas
Ideal Gas Law
The ideal gas law is a cornerstone of thermodynamics, providing a relationship between the pressure, volume, and temperature of an ideal gas. This law is expressed by the equation \( PV = nRT \), where:
- \( P \) represents the pressure of the gas.
- \( V \) indicates the volume of the gas.
- \( n \) is the number of moles of the gas.
- \( R \) is the universal gas constant \( (8.314 \,\mathrm{J\,mol^{-1}\,K^{-1}}) \).
- \( T \) is the temperature in Kelvin.
Molar Heat Capacity
Molar heat capacity is a measure of the amount of heat required to increase the temperature of one mole of a substance by one degree Celsius (or one Kelvin). It is denoted by \( C \) and is expressed in units of \( \mathrm{J/mol\, °C} \) or \( \mathrm{J/mol\, K} \).
The molar heat capacity at constant pressure \( C_p \) is especially important when dealing with gases like helium in our example. Here, the molar heat capacity of helium gas is given as \( 20.8 \,\mathrm{J/mol\,°C} \).
Using the relationship \( q = nC_p \Delta T \), where:
The molar heat capacity at constant pressure \( C_p \) is especially important when dealing with gases like helium in our example. Here, the molar heat capacity of helium gas is given as \( 20.8 \,\mathrm{J/mol\,°C} \).
Using the relationship \( q = nC_p \Delta T \), where:
- \( q \) is the heat absorbed or released.
- \( n \) indicates the number of moles.
- \( \Delta T \) is the change in temperature, obtained by subtracting the initial temperature from the final temperature (in Kelvin).
Internal Energy
Internal energy (\( \Delta E \)) refers to the total energy contained within a thermodynamic system. It represents the sum of the potential and kinetic energy of the molecules in the system. Changes in internal energy correspond to the energy added or removed from the system, either by heat transfer or by doing work.
The first law of thermodynamics is key to understanding internal energy changes and is stated as \( \Delta E = q + w \). Here:
The first law of thermodynamics is key to understanding internal energy changes and is stated as \( \Delta E = q + w \). Here:
- \( q \) is the heat exchanged with the surroundings.
- \( w \) is the work done by or on the system.
Work Done by Gas
In thermodynamics, work done by a gas during its expansion or compression is an important concept. When a gas does work, its internal energy changes, often along with other state variables such as volume, pressure, and temperature. The work done by a gas is calculated using the equation \( w = -P \Delta V \), especially in constant pressure scenarios.
- \( P \) is the pressure of the gas (constant in this problem).
- \( \Delta V \) is the change in volume, the difference between the final and initial volumes.
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