The First Law of Thermodynamics: Control Volumes

 Here we will extend the conservation of energy to systems that involve mass flow across their boundaries, control volumes. Any arbitrary region in space can be selected as control volume. There are no concrete rules for the selection of control volumes. The boundary of control volume is called a control surface. 



Conservation of Mass Like energy, mass is a conserved property, and it cannot be created or destroyed. Mass and energy can be converted to each other according to Einstein’s formula: E = mc2 , where c is the speed of light. However, except for nuclear reactions, the conservation of mass principle holds for all processes.   For a control volume undergoing a process, the conservation of mass can be stated as: total mass entering CV – total mass leaving CV = net change in mass within CV mi me  mCV



The conservation of mass can also be expressed in the rate form: m m dm dt CV  i  e  /   The amount of mass flowing through a cross section per unit time is called the mass flow rate and is denoted by m°. The mass flow rate through a differential area dA is: dm°= ρVn dA where Vn is the velocity component normal to dA. Thus, the mass flow rate for the entire cross‐section is obtained by:



A process during which a fluid flows through a control volume steadily is called steady‐ state process. A large number of devices such as turbines, compressors, and nozzles operates under the same conditions for a long time and can be modeled (classified) as steady‐flow devices.   The term steady implies no change with time. The term uniform implies no change with location over a specified region. A steady flow is characterized by the following:  

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