Thermodynamics Questions for Helium and Flourine

In summary, the conversation discusses a student seeking help with physics over the summer and provides two problems involving calculations for the average translational kinetic energy, velocity, and total internal energy of helium and fluorine molecules at different temperatures and molar masses. The student also mentions relevant equations and concepts needed to solve the problems.
  • #1
Tofuphysics
1
0
Hey all, I just discrovered these forums, thankoodness, because I'm taking physics over the summer (its a requirement at my school), and not being a science-y person, I really need help.

Homework Statement

[/B]

This is the problem:

Problem 1
a. What is the average translational kinetic energy of a helium atom at 300 K?
b. What is the average translational velocity of a helium atom at 300 K?
c. What is the total internal energy of a 4.0 g sample of He at 300 K?
d. What is the total internal energy of a 4.0 g sample of He at 301 K?
e. How much energy is needed to raise the temperature of 4.0 g of He by one degree K?

And then the next problem is he same cocept, but with Flourine (F2)

Problem 2
a. What is the average translational kinetic energy of a F2 molceule at 300 K?
b. What is the average translational velocity of a F2 moelcule at 300 K?
c. What is the total internal energy of a 38 g sample of F2 at 300 K?
d. What is the total internal energy of a 38 g sample of F2 at 301 K?
e. How much energy is needed to raise the temperature of 38 g of F2 by one degree K?

Homework Equations


KE=(3/2)(Kb)(T)
KE=1/2mv^2
Avogadroes number= 6.02 x 10^-23
1 MW= 1x wx^6 w (i don't know what this means but the teacher wrote it on the board)

The Attempt at a Solution


I think that you have to use the KE equations and the molar mass (which you can figure out using the periodic table?) but I'm really not sure how to put it together.


Thankyou so much if you had the patience to read all that!
-Tofuphysics
 
Last edited:
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  • #2
Welcome to PF Tofuphysics,
Tofuphysics said:
KE=(3/2)(Kb)(T)
KE=1/2mv^2
Avogadroes number= 6.02 x 10^-23
Assuming of course that you are treating these gases as ideal, then those equations are correct and will certainly allow you to answer questions (a) and (b) in each case. However, a third equation would be infinitely more useful in answering the remaining parts.
 
  • #3


Hello Tofuphysics,

I'm glad you found these forums to help you with your physics homework! Let's go through the questions one by one and see if we can figure out the answers together.

a. The average translational kinetic energy of a helium atom at 300 K can be calculated using the equation KE=(3/2)(Kb)(T). Kb represents the Boltzmann constant, which is equal to 1.38x10^-23 J/K. T is the temperature in Kelvin, so for 300 K, we get:

KE = (3/2)(1.38x10^-23 J/K)(300 K) = 6.21x10^-21 J

b. To find the average translational velocity of a helium atom, we can use the equation KE=1/2mv^2. Rearranging this equation, we get v = √(2KE/m). Plugging in the value for KE from part a and the mass of a helium atom (4.0 g/mol), we get:

v = √(2(6.21x10^-21 J)/(4.0 g/mol)) = 8.77x10^2 m/s

c. The total internal energy of a 4.0 g sample of He at 300 K can be calculated by multiplying the average translational kinetic energy from part a by the number of atoms in the sample. The molar mass of He is 4.0 g/mol, so there are 1 mol of atoms in 4.0 g of He. Using Avogadro's number (6.02x10^23 atoms/mol), we get:

Total internal energy = (6.21x10^-21 J/atom)(6.02x10^23 atoms/mol) = 3.74x10^3 J

d. To find the total internal energy of a 4.0 g sample of He at 301 K, we can use the same method as in part c, but with the new average translational kinetic energy at 301 K. This value can be calculated using the equation KE=(3/2)(Kb)(T) as in part a. The total internal energy at 301 K will be slightly higher than at 300 K.

e. The amount of energy needed to raise the temperature of 4.0 g of He by one degree K can be
 

Related to Thermodynamics Questions for Helium and Flourine

1. What is the difference between helium and fluorine in terms of their thermodynamic properties?

Helium and fluorine have very different thermodynamic properties. Helium is a noble gas and has very low boiling and melting points, making it useful for applications such as cooling and as a lifting gas. Fluorine, on the other hand, is a highly reactive gas with a much higher boiling point and is used in applications such as refrigerants and as a reactant in chemical reactions.

2. How do the thermodynamic properties of helium and fluorine affect their behavior under different temperature and pressure conditions?

The thermodynamic properties of helium and fluorine play a crucial role in their behavior under different temperature and pressure conditions. For example, helium remains a gas at very low temperatures and high pressures, while fluorine can become a liquid or solid under these conditions due to its higher boiling point and reactivity.

3. Can helium and fluorine be used together in thermodynamic systems?

Yes, helium and fluorine can be used together in thermodynamic systems. Helium is often used as a refrigerant in combination with fluorine-based refrigerants, and fluorine compounds can also be used as catalysts for reactions involving helium gas.

4. How does the thermodynamic behavior of helium and fluorine impact their use in industry?

The unique thermodynamic properties of helium and fluorine make them valuable resources for various industries. Helium is used in applications such as cooling, welding, and as a lifting gas, while fluorine is used in refrigerants, semiconductor manufacturing, and as a reactant in chemical reactions.

5. Can the thermodynamic properties of helium and fluorine change over time?

Yes, the thermodynamic properties of helium and fluorine can change over time. For example, helium can become contaminated with other gases over time, which can affect its behavior in thermodynamic systems. Additionally, fluorine can undergo chemical reactions that can alter its properties, making it important to monitor and control its use in industrial processes.

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