in brief...
- molecules of methane are bonded by dispersion forces
- dispersion forces are the weakest form of intermolecular bonding, meaning that there is only a small amount of energy (or heat) required to break the weak dispersion forces between the methane molecules
- because there is not much heat required to break dispersion forces - we can understand why methane boils so easily and at such a low temperature
[explanation of dispersion forces in more detail...
- electrons inside an atom move around the nucleus randomly
- it is likely that, at any one instant, there may be more electrons on one side of the nucleus than the other
- this results in one side of the atom being more negatively charged than the other at this instant (the side with more electrons on it than the other would obviously be more negatively charged)
- now to explain how this applies to intermolecular bonding...well - to make things easier, I'll name one molecule BOB and another STEVE. imagine that STEVE is standing to BOB's left. if say, we froze time - and at that instant there were more electrons on the left hand side of BOB's body - the left hand side of BOB would become negatively charged. the electrons inside STEVE (who is standing to BOB's left) would suddenly be repelled to his left, as far away from the negative side of BOB as possible. thus the right hand side of STEVE would become positively charged while the left hand side of STEVE would become negatively charged just like BOB. this would continue on in a domino kind of a way to surrounding molecules - and the attraction between the negatively charged side of BOB and the positively charged side of STEVE is what we call dispersion forces.
in more scientific terms: dispersion forces are the attraction that exists between molecules because of the temporary dipoles (differences in charge of one side of a molecule to the other) that form as electrons move randomly
- dispersion forces are very, very weak - which explains why molecules that are bonded in this form have such low boiling temperatures]
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in brief...
- molecules of methane are bonded by dispersion forces
- dispersion forces are the weakest form of intermolecular bonding, meaning that there is only a small amount of energy (or heat) required to break the weak dispersion forces between the methane molecules
- because there is not much heat required to break dispersion forces - we can understand why methane boils so easily and at such a low temperature
[explanation of dispersion forces in more detail...
- electrons inside an atom move around the nucleus randomly
- it is likely that, at any one instant, there may be more electrons on one side of the nucleus than the other
- this results in one side of the atom being more negatively charged than the other at this instant (the side with more electrons on it than the other would obviously be more negatively charged)
- now to explain how this applies to intermolecular bonding...well - to make things easier, I'll name one molecule BOB and another STEVE. imagine that STEVE is standing to BOB's left. if say, we froze time - and at that instant there were more electrons on the left hand side of BOB's body - the left hand side of BOB would become negatively charged. the electrons inside STEVE (who is standing to BOB's left) would suddenly be repelled to his left, as far away from the negative side of BOB as possible. thus the right hand side of STEVE would become positively charged while the left hand side of STEVE would become negatively charged just like BOB. this would continue on in a domino kind of a way to surrounding molecules - and the attraction between the negatively charged side of BOB and the positively charged side of STEVE is what we call dispersion forces.
in more scientific terms: dispersion forces are the attraction that exists between molecules because of the temporary dipoles (differences in charge of one side of a molecule to the other) that form as electrons move randomly
- dispersion forces are very, very weak - which explains why molecules that are bonded in this form have such low boiling temperatures]
The molecule with a high vapor pressure is the molecule with the weaker intermolecular forces. Water has all three intermolecular forces, london dispersion forces, hydrogen bondings, and dipole-dipole forces. Methane, on the other hand, has only london dispersion forces because it is nonpolar. Moreover, we have to consider molecular weights. The molecule with a larger molecular weight will have more london forces involved in bonding in order to stabilize the molecule, and hence would have stronger intermolecular forces because all the weak forces (london forces) will behave as strong forces. Both molecules have similar molecular weights, so we can't compare which molecular is larger. Hence, we have to consider the molecule with the strongest intermolecular force. Hydrogen bondings are the strongest intermolecular forces, and they are seen in water. Thus, water has stronger intermolecular forces. So, the molecule with weaker intermolecular forces is methane, and thus has a higher vapor pressure.
The vapor density of an equimolar mixture of methane (CH4) and oxygen (O2) would be the average of the individual vapor densities of methane and oxygen. The vapor density of methane is approximately 8 g/L and oxygen is approximately 16 g/L, so the equimolar mixture would have a vapor density close to 12 g/L.
The vapor pressure graph shows that as temperature increases, the vapor pressure also increases. This indicates a direct relationship between temperature and vapor pressure, where higher temperatures result in higher vapor pressures.
The vapor pressure of water at 50°C is the same as the vapor pressure at 50°C. Vapor pressure is a function of temperature and does not change for a substance at a specific temperature.
The vapor pressure is the pressure exerted by a vapor in thermodynamic equilibrium with its condensed phases at a given temperature. The vapor pressure depends on the temperature and the substance.
The vapor pressure vs temperature graph shows that as temperature increases, the vapor pressure also increases. This indicates that there is a direct relationship between vapor pressure and temperature, where higher temperatures lead to higher vapor pressures.
Ozone, Methane, Water vapor.
The vapor density of an equimolar mixture of methane (CH4) and oxygen (O2) would be the average of the individual vapor densities of methane and oxygen. The vapor density of methane is approximately 8 g/L and oxygen is approximately 16 g/L, so the equimolar mixture would have a vapor density close to 12 g/L.
The vapor pressure graph shows that as temperature increases, the vapor pressure also increases. This indicates a direct relationship between temperature and vapor pressure, where higher temperatures result in higher vapor pressures.
The vapor pressure of water at 50°C is the same as the vapor pressure at 50°C. Vapor pressure is a function of temperature and does not change for a substance at a specific temperature.
The vapor pressure is the pressure exerted by a vapor in thermodynamic equilibrium with its condensed phases at a given temperature. The vapor pressure depends on the temperature and the substance.
The vapor pressure vs temperature graph shows that as temperature increases, the vapor pressure also increases. This indicates that there is a direct relationship between vapor pressure and temperature, where higher temperatures lead to higher vapor pressures.
True Vapor Pressure is the pressure of the vapor in equilibrium with the liquid at 100 F (it is equal to the bubble point pressure at 100 F)
Mainly ammonia, methane, and water vapor.
Another name for gas is vapor.
The term is "boiling point." At this temperature, liquid changes to vapor as its vapor pressure is equal to the atmospheric pressure.
The maximum pressure of vapor that can build up in a closed container is the vapor pressure of the substance at the given temperature. Once the vapor pressure is reached, the system reaches equilibrium and no further increase in pressure occurs. Any additional vapor will condense back into liquid form.
To determine the mole fraction from vapor pressure, you can use Raoult's Law. This law states that the vapor pressure of a solution is directly proportional to the mole fraction of the solvent in the solution. By measuring the vapor pressure of the solution and knowing the vapor pressure of the pure solvent, you can calculate the mole fraction of the solvent in the solution using the formula: Mole fraction of solvent Vapor pressure of solution / Vapor pressure of pure solvent