Electric calorimeter , steam Formation, 2D ,3D graph , all are included in this ppt.
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Steam Formation Unit - 4
Some important terms Liquid that is not about to vaporize, is called Compressed liquid. Liquid that is about to vaporize, is called Saturated liquid.
A vapour that is about to condense is called Saturated vapor . A vapor that is not about to condense (i.e., not a saturated vapor ) is called a superheated vapor .
At a given pressure, the temperature at which a pure substance changes phase is called the saturation temperature Tsat . Likewise, at a given temperature, the pressure at which a pure substance changes phase is called the saturation pressure Psat .
P-V diagram
Formation of steam
Graphical representation of formation of steam
h-s Diagram or Mollier Diagram P=c
IMPORTANT TERMS RELATING STEAM FORMATION Sensible heat of water ( h f ) It is defined as the quantity of heat absorbed by 1 kg of water when it is heated from 0°C (freezing point) to boiling point. It is also called total heat (or enthalpy) of water or liquid heat invariably. Latent heat or hidden heat ( h fg ). It is the amount of heat required to convert water at a given temperature and pressure into steam at the same temperature and pressure. It is expressed by the symbol h fg .
Superheated steam. When steam is heated after it has become dry and saturated, it is called superheated steam and the process of heating is called superheating. Superheating is always carried out at constant pressure. The additional amount of heat supplied to the steam during superheating is called as ‘ Heat of superheat’ Total heat or enthalpy of wet steam (h). It is defined as the quantity of heat required to convert 1 kg of water at 0°C into wet steam at constant pressure. It is the sum of total heat of water and the latent heat and this sum is also called enthalpy. Where C ps is the specific heat of superheated steam at constant pressure.
Dryness fraction or Quality (x). The term dryness fraction is related with wet steam. It is defined as the ratio of the mass of water vapour in steam to the mass of steam containing it. It is usually expressed by the symbol ‘x’ or ‘q’. Where m g and m l are the masses of vapour and liquid respectively in the mixture.
We can also write
Constant quality lines
Steam table is a tabular presentation of properties such as specific enthalpy, entropy, internal energy and specific volume at different saturation pressures and temperatures. Steam table may be on pressure basis or on temperature basis. The table on pressure basis has continuous variation of pressure and corresponding to it : saturation temperature ( Tsat ), enthalpy of saturated liquid ( h f ), enthalpy of saturated vapour (h g ), entropy of saturated liquid ( s f ), entropy of saturated vapour ( sg ), specific volume of saturated liquid ( v f ), specific volume of saturated vapour ( vg), internal energy of saturated liquid ( u f ), internal energy of saturated vapour ( u g ) are given on unit mass basis. Steam Tables
Dryness fraction measurement: In the measurement of quality, the object is always to bring the state of the substance from the two-phase region to the single-phase or superheated region, where both pressure and temperature are independent. It can be measured either by adiabatic throttling or electric heating.
Throttling calorimeter: In the throttling calorimeter, a sample of wet steam of mass m and at pressure p 1 is taken from the steam main through a perforated sampling tube. Then it is throttled by the partially-opened valve to a pressure p 2 , measured by mercury manometer, and temperature t 2 , so that after throttling the steam is in the superheated region.
The initial state (wet) is given by p1 and x1, and the final state by p 2 and t 2 (superheated). Now With p 2 and t 2 being known, h 2 can be found out from the superheated steam table. The values of h 1 and h fgp1 are taken from the saturated steam table corresponding to pressure p i . Therefore, the quality of the wet steam x i can be calculated.
Electric calorimeter: The sample of steam is passed in steady flow through an electric heater, as shown. The electrical energy input Q should be sufficient to take the steam to the superheated region where pressure p 2 and temperature t 2 are measured. If I is the current flowing through the heater in amperes and V is the voltage across the coil, then at steady state Q = VI x 10 -3 kW. If m is the mass of steam taken in t seconds under steady flow condition, then the steady flow energy equation for the heater (as control volume) gives
w 1 h 1 + Q = w 1 h 2 where w 1 is the steam flow rate in kg/s (w 1 = m/t kg/s) So, h 1 + Q/ w 1 = h 2 With h 2 , Q and w 1 being known, h1 can be computed. Now h 1 = h fp1 + x 1 h fgp1 Hence x 1 can be evaluated.