Thermo-Fluids ERE 221 Lecture 2: Introduction - Energy Dr. Ahmed Elwardany Energy Resources Engineering (ERE) Department Email: ahmed.Elwardany@ejust.edu.eg Atef Last lecture • • • • • Introduction: history Types of thermodynamics Units and Dimensions Systems Property, State, Process and Cycle Atef 2 Temperature and Zeroth Law of T.D How could we define it? A measure of hotness or coldness. It determines whether they will be in thermal equilibrium Freezing cold, cold, warm, hot, and red-hot (Sensation) A metal chair will feel much colder than a wooden one even when both are at the same temperature ! Two bodies at different T Heat is transferred from the body at higher T to the one at lower T until both bodies attain the same temperature. The heat transfer stops, and the two bodies are said to have reached thermal equilibrium. Two bodies at different T The zeroth law of thermodynamics states that if two bodies are in thermal equilibrium with a third body, they are also in thermal equilibrium with each other. Atef 3 Temperature Scales All temperature scales are based on some easily reproducible states such as the freezing and boiling points of water, which are also called the ice point and the steam point, respectively. Temperature scales are defined by the numerical value assigned to a standard fixed point. By international agreement the standard fixed point is the easily reproducible triple point of water: the state of equilibrium between steam, ice, and liquid water. The triple point of pure water is at 0.01°C (273.16 K, 32.01°F) The ice point is (273.15 K) The steam point is (373.15 K) Atef 4 Temperature Scales The Rankine scale is The temperature scales in the two unit systems Atef 5 Temperature Rise During a heating process, the temperature of a system rises by 10°C. Express this rise in temperature in K, °F, and R. Atef 6 Pressure Pressure is defined as a normal force exerted by a fluid per unit area. P=F/A (Pa = N/m2) Absolute pressure: The actual pressure at a given position, and it is measured relative to absolute vacuum (i.e., absolute zero pressure). Most pressure-measuring devices, however, are calibrated to read zero in the atmosphere. Gage pressure is the difference between the absolute pressure and the local atmospheric pressure and measured by pressure gages. Pgage can be positive or negative, but pressures below atmospheric pressure are sometimes called vacuum pressures Atef 7 Pressure Atmospheric pressure: represents the weight of the atmosphere around us. (standard pressure=101.3 kPa) Dr Ahmed Elwardany, ERE, Spring 2019 Atef 8 Pressure: example A vacuum gage connected to a chamber reads 5.8 psi at a location where the atmospheric pressure is 14.5 psi. Determine the absolute pressure in the chamber. Atef 9 Pressure: with Depth Atef 10 Pressure: with Depth Atef 11 Atmospheric Pressure The Barometer The pressure at point B is equal to the atmospheric pressure, and the pressure at point C can be taken to be zero since there is only mercury vapor above point C and the pressure is very low relative to Patm and can be neglected to an excellent approximation. The standard atmospheric pressure is 760 mmHg (29.92 in Hg) at 0°C. The unit mmHg is also called the torr in honor of Torricelli. Therefore, 1 atm = 760 torr and 1 torr = 133.3 Pa. The length or the cross-sectional area of the tube has no effect on the height of the fluid column of a barometer Atef 12 Energy Energy (E) Energy is defined as the capacity of a system to perform work or produce heat. Energy exists in numerous forms such as thermal, mechanical, electric, chemical, and nuclear. Even mass can be considered a form of energy. Energy can be transferred to or from a closed system (a fixed mass) in two distinct forms: heat and work. An energy transfer to or from a closed system is heat if it is caused by a temperature difference. Otherwise it is work, and it is caused by a force acting through a distance. For control volumes, energy can also be transferred by mass flow. Atef 13 Forms of Energy The total energy of a system on a unit mass basis is denoted by e and is expressed as Thermodynamics provides no information about the absolute value of the total energy. It deals only with the change of the total energy, which is what matters in engineering problems. Atef 14 Forms of Energy Energy Work Energy Heat Energy Internal Energy Flow Energy Potential energy Kinetic energy Atef 15 Forms of Energy The various forms of total energy could be considered a system in two groups: macroscopic and microscopic. The macroscopic forms of energy are those a system possesses as a whole with respect to some outside reference frame, such as kinetic and potential energies. The microscopic forms of energy are those related to the molecular structure of a system and the degree of the molecular activity, and they are independent of outside reference frames. The sum of all the microscopic forms of energy is called the internal energy of a system and is denoted by U. Atef 16 Kinetic Energy (KE) KE is the energy that a system possesses as a result of its motion relative to some reference frame The kinetic energy is expressed as or, on a unit mass basis, V: Velocity (m/s) m: Mass (kg) Atef 17 Potential Energy (PE) PE is the energy that a system possesses as a result of its elevation in a gravitational field The potential energy is expressed as or, on a unit mass basis, g: Gravitational acceleration (9.81 m/s2) z: Elevation of the center of gravity of a system relative to reference level. Atef 18 Internal Energy (U) Internal energy is the sum of all the microscopic forms of energy of a system. It is related to the molecular structure and the degree of molecular activity, and can be viewed as the sum of the kinetic and potential energies of the molecules. Translational energy: molecules of a gas move through space with some velocity, and thus possess some kinetic energy. Rotational and vibrational energy: for polyatomic molecules. Electron spin and in an atom rotate about the nucleus, and thus possess rotational kinetic energy. Electrons at outer orbits have larger kinetic energies. Electrons also spin about their axes, and the energy associated with this motion is the spin energy. Atef 19 Energy Total Energy Stationary system: A closed system its velocity and elevation of the center of gravity remain constant during a process. Control volumes typically involve fluid flow for long periods of time, and it is convenient to express the energy flow associated with a fluid stream in the rate form. Atef 20 Flow Energy (FE) It arises from the pressure (P) and the volume (V) of a fluid. FE = where: P = pressure (kN/m2) V = total volume (m3) v = specific volume (m3/kg) m = mass (kg). Atef 21 Enthalpy (H) Enthalpy is a property of a substance, like pressure, temperature, and volume, but it cannot be measured directly. Normally, the enthalpy of a substance is given with respect to some reference value. h = u + P v = internal energy + flow energy Flow energy means that enthalpy appear when dealing with open systems For ideal gases: h = cp T (kJ/kg) u = cv T (kJ/kg) Atef 22 Mechanical Energy The form of energy that can be converted to mechanical work completely and directly by an ideal mechanical device such as an ideal turbine. Kinetic and potential energies are the familiar forms of mechanical energy. Thermal energy is not mechanical energy. The mechanical energy of a flowing fluid Atef 23 Example A site evaluated for a wind farm is observed to have steady winds at a speed of 8.5 m/s. Determine the wind energy (a) per unit mass, (b) for a mass of 10 kg, and (c) for a flow rate of 1154 kg/s for air. Atef 24 Thank You! Atef