When heat is added to a saturated vapor, its temperature will increase and the vapor will start to undergo phase change into a superheated vapor. This means that the vapor will contain more thermal energy than at saturation conditions, which leads to a rise in temperature without a change in pressure.
Latent heat is released when water vapor condenses in saturated air. Therefore, the most latent heat would be released in a parcel of saturated air when the water vapor in the air condenses into liquid water, such as during the process of cloud formation or precipitation.
Adding heat to water vapor will just cause the molecules to gain energy and move faster. As long as the amount of energy added is not extraordinary, this is all that will happen. At extremely high temperatures, the water vapor may convert to hydrogen and oxygen gas.
Because to perform the change of state from the saturated liquid to saturated vapor ( at constant presure ) you have to add heat in the amount of the substance's evaporation latent heat Qev . At constant pressure, temperature will stay fixed at its saturation temperature and the increase in entropy will be (delta S)ev = Qev/Tsat where (delta S)ev is the entropy increment. Tsat is the saturation absolute temperature of the substance. And so the saturated vapor entropy is (delta S)ev larger than the saturated liquid entropy.
Adding heat to a vapor after the change of state from liquid to vapor has occurred is called super-heating. For example, adding heat to steam at 100 C and 101.325 kPa is called super-heating.
When water evaporates, heat from the surroundings is absorbed to break the bonds between water molecules, turning liquid water into water vapor. This heat energy is stored in the water vapor as latent heat, increasing its kinetic energy.
The heat added to a saturated vapor to raise its temperature above its boiling point is referred to as sensible heat. This is because the heat causes a change in temperature without a phase change.
Latent heat is released when water vapor condenses in saturated air. Therefore, the most latent heat would be released in a parcel of saturated air when the water vapor in the air condenses into liquid water, such as during the process of cloud formation or precipitation.
Any addition of thermal energy to a saturated liquid will cause it to vaporize. Any subtraction of thermal energy from a saturated vapor will cause it to condense.
A condenser rejects heat to the environment to turn vapor into liquid. Ideally a vapor enters the condenser as saturated vapor, meaning it's at the boiling point. The vapor condenses and leaves the condenser at saturated liquid (also at the boiling temperature).
Adding heat to water vapor will just cause the molecules to gain energy and move faster. As long as the amount of energy added is not extraordinary, this is all that will happen. At extremely high temperatures, the water vapor may convert to hydrogen and oxygen gas.
Air can become saturated by reaching its dew point temperature, which is the temperature at which the air can no longer hold all of its moisture and water vapor begins to condense into liquid form. When this happens, the air is at 100% relative humidity and is considered saturated.
When water vapor is added to dry air, the humidity of the air increases. This can lead to the air feeling warmer because water vapor traps heat, and can also contribute to the formation of clouds and precipitation if the air reaches its saturation point.
When heat is added to a substance, the molecules and atoms vibrate faster.
Adding heat to a vapor after the change of state from liquid to vapor has occurred is called super-heating. For example, adding heat to steam at 100 C and 101.325 kPa is called super-heating.
Because to perform the change of state from the saturated liquid to saturated vapor ( at constant presure ) you have to add heat in the amount of the substance's evaporation latent heat Qev . At constant pressure, temperature will stay fixed at its saturation temperature and the increase in entropy will be (delta S)ev = Qev/Tsat where (delta S)ev is the entropy increment. Tsat is the saturation absolute temperature of the substance. And so the saturated vapor entropy is (delta S)ev larger than the saturated liquid entropy.
it bubbled, evaporates,
Temperature rises, liquid starts boiling becoming vapor