Temperature is used as for measuring the average kinetic energy present in a substance or object.
The internal kinetic energy obtained by the molecules of an object is known as thermal energy.
Hence, temperature measures the thermal energy of an object.
Whereas when this thermal energy flows from a hotter object to a cooler object which are placed adjacent to each other then it is known that heat is flowing.
Thus, we can conclude that heat differ from temperature as temperature measures thermal energy, and heat is the flow of thermal energy.
The exit temperature of the Nitrogen would be 331.4 K.
The area at the exit of the diffuser would be .
The rate of entropy production would be 0.
Explanation:
First it is assumed that the diffuser works as a isentropic device. A isentropic device is such that the entropy at the inlet is equal that the entropy T the exit.
It will be used the subscript <em>1 for the</em> <em>inlet conditions of the nitrogen</em>, and the subscript <em>2 for the exit conditions of the nitrogen</em>.
It will be called: <em>v</em> the velocity of the nitrogen stream, <em>T</em> the nitrogen temperature, <em>V</em> the volumetric flow of the specific stream, <em>A</em> the area at the inlet or exit of the diffuser and, <em>P</em> the pressure of the nitrogen flow.
It is known that <em>for a fluid flowing, its volumetric flow is obtain as:</em> ,
Then for the inlet of the diffuser:
For an ideal gas working in an isentropic process, it follows that: where each variable is defined according with what was presented in step 2 and 3, and <em>k </em>is the heat values relationship, 1.4 for nitrogen.
Then <em>solving</em> for , the temperature of the nitrogen at the exit conditions: then,
Also, for an ideal gas working in an isentropic process, it follows that: , where each variable is defined according with what was presented in step 2 and 3, and <em>k</em> is the heat values relationship, 1.4 for nitrogen.
Then <em>solving</em> for the volumetric flow at the exit of the diffuser: .
Knowing that , it is possible to calculate the area at the exit of the diffuser, using the relationship presented in step 4, and solving for the required parameter: .
<em>To determine the rate of entropy production in the diffuser,</em> it is required to do a second law balance (entropy balance) in the control volume of the device. This balance is: , where: and are the entropy of the stream entering and leaving the control volume respectively, is the rate of entropy production and, is the change of entropy of the system.
If the diffuser is operating at stable state is assumed then . Applying the entropy balance and solving the rate of entropy generation: .
Finally, it was assume that the process is isentropic, it is: , then .
A gaseous solute will <span> be able to be dissolve in a liter of liquid water by increasing the pressure of the gas. an example of this situation is the increase in solubility of carbon dioxide in sea water which turns it into an acidic environment for marines as pressure increases.</span>