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 ...
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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

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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

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Heating - History 700 BC - 0

Hypocausta

Michal Kabrhel

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Heating - History – Middle Ages n

Fireplace, stove

BEE1 Michal - prof.Kabele Kabrhel

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Heating - History 18th-19th century - steam system

Michal Kabrhel

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Heating - History 20thcentury

Michal Kabrhel

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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

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1900-1945

Michal Kabrhel

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Heating nowadays n n n n

Warm water systems Gas boilers operated by electronics Heating surface inside floor, wall, ceiling Computer models

Michal Kabrhel

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Heating nowadays

Michal Kabrhel

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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

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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

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Basic laws of thermodynamics n

1.law n

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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

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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

2008/2009

Michal Kabrhel

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Heat transfer n

Transmission convection+conduction+convection

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Radiation n Electromagnetic waves

2008/2009

Michal Kabrhel

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Indoor environment

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Theory of the indoor environment n n n n n

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Hygrothermal microclimate Acoustic microclimate Psychical microclimate Light microclimate Electrostatic microclimate

Hygrothermal microclimate n

2008/2009

Indoor environment state from the viewpoint of thermal and moisture flows between the human body and surroundings

Michal Kabrhel

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Heat Exchange between the Human Body and the Enviroment n

Metabolic Rate M n n n

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n n n n

T p

Heat loss Q n

n

degree of muscular activities, environmental conditions body size.

T

Respiration Convection Radiation Conduction Evaporation

a

Body thermal balance equation

2008/2009

M=Q comfort M>Q hot M50

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