Czech Technical University in Prague Faculty of Civil Engineering Department of Microenvironmental and Building Services Engineering
Czech Technical University in Prague Faculty of Civil Engineering Department of Microenvironmental and Building Services Engineering
Heating systems ...
Czech Technical University in Prague Faculty of Civil Engineering Department of Microenvironmental and Building Services Engineering
Heating systems Apllied thermodynamics Indoor environment
2008/2009
Michal Kabrhel
1
Heating n
The function Heat supply to guarantee required indoor temperature n Heat supply for technology n Heat supply for hot water generation n
n
The principle
Michal Kabrhel
2
Heating - History 700 BC - 0
Hypocausta
Michal Kabrhel
3
Heating - History – Middle Ages n
Fireplace, stove
BEE1 Michal - prof.Kabele Kabrhel
4
Heating - History 18th-19th century - steam system
Michal Kabrhel
5
Heating - History 20thcentury
Michal Kabrhel
6
th 20 century
History warm water systems Steam systems are replaced by warm water ones - use of electricity, pumps, control
Michal Kabrhel
Warm water boiler Strebl 1927
7
1900-1945
Michal Kabrhel
8
Heating nowadays n n n n
Warm water systems Gas boilers operated by electronics Heating surface inside floor, wall, ceiling Computer models
Michal Kabrhel
9
Heating nowadays
Michal Kabrhel
10
Applied thermodynamics n
Heat, heat energy n
n
Heat is the energy transferred between a system and its surroundings due solely to a temperature difference between the system and some parts of its surroundings.
Temperature n
State variable describing kinetics energy of the particles of the system n n n
2008/2009
Thermodynamic /Kelvin/ T [K] Celsius t [°C] t= T-273,15 Fahrenheit [°F] 1°F=5/9°C (°F-32).5/9=°C
Michal Kabrhel
11
Basic laws of thermodynamics n
Zeroth law n
n
2008/2009
There is a state variable TEMPERATURE. Two systems at the same temperature are in thermodynamics equilibrium. The zeroth law of thermodynamics states that if for example you have a Body (A) and a Body (B), both at the same temperature; and then you have a Body (C) which is at the same temperature as Body (B); Therefore the temperature of Body (C) is equal to the temperature of Body (A).
Michal Kabrhel
12
Basic laws of thermodynamics n
1.law n
n
2.law n
n
The total energy of the system plus the surroundings is constant. (internal energy of system) The second law is concerned with entropy (S), which is a measure of disorder. The entropy of the universe increases.
3.law n
2008/2009
It is impossible to cool a body to absolute zero by any finite process
Michal Kabrhel
13
Heat transfer modes n
Heat Conduction n
n
Heat is transferred between two systems through a connecting medium, Biot-Fourier
Heat Convection Macroscopic movement of the matter in the forms of convection currents. n Newton-Richman, Fourier-Kirchhof n