THERMAL LOADING OF BUILDINGS

Slides:



Advertisements
Similar presentations
Section 6. HEAT TRANSFER Dr. Congxiao Shang.
Advertisements

HEAT LOSS & HEAT GAIN HEAT FLOW. Heat flows from high temperature to low temperature There are 3 types/methods of heat flow/transfer: 1.Conduction- through.
Application of Steady-State Heat Transfer
The Three Tiered Philosophy
UNIT 13 : HEAT 13.1 Thermal Conductivity 13.2 Thermal Expansion.
Heat transfer rates through a bedroom window with and without an A/C unit Sam Sanderson David Theurer December 2006.
So Far: Conservation of Mass and Energy Pressure Drop in Pipes Flow Measurement Instruments Flow Control (Valves) Types of Pumps and Pump Sizing This Week:
Matter and Energy.
Heat Transfer Chapter 2.
1 ISAT Module III: Building Energy Efficiency Topic 6:Stead-State Building Loads z Fabric Loss z Ventilation Loss z Environmental Temperature z Steady-State.
Chapter 2: Overall Heat Transfer Coefficient
One-Dimensional Steady-State Conduction
Heat Loss & Gain Calculations 1. How Heat Moves in Homes Conduction is the transfer of heat through solid objects, such as the ceilings, walls, and floors.
Furnace Efficiency Bryce Cox Dallin Bullock. Problem My gas bill is very expensive My furnace claims an efficiency of 78% but it appears to be less efficient.
DR.PRADIP DUTTA Department of Mechanical Engineering Indian Institute of Science Bangalore.
 Site  Requirements  Local Resources  Initial layout ideas  Brief material selection  Supply options.
Temperature and Heat Loss The following topics are covered in this presentation: Temperature and temperature scales Transfer of heat Thermal conductivity,
Conduction & Convection.
Heat Loss and Gain Heat Loss and Gain
The Buildings Envelope.  R Values are the thermal resistance of a building product. R values are given to certain materials to evaluate there ability.
P1a 1.5 Heat transfer by design. Lesson Objectives To investigate factors that affect the rate of thermal energy transfer. To describe how thermal energy.
ISAT Module III: Building Energy Efficiency
Climate and Architecture Dr. Abdelrahman Elbakheit
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Chapter 3 Part 1 One-Dimensional, Steady-State Conduction.
So Far: Conservation of Mass and Energy Pressure Drop in Pipes Flow Measurement Instruments Flow Control (Valves) Types of Pumps and Pump Sizing This Week:
HVACR416 - Design Heat Loss / Heat Gain Part 1. Why? The primary function of Air Conditioning is to maintain conditions that are… o Conductive to human.
1 ISAT Module III: Building Energy Efficiency Topic 7: Transient Heating and Air Conditioning Loads  Thermal Admittance  Intermittent Heating 
Remember... Resistance in Mechanical systems (friction) opposes motion of solid objects.
One-Dimensional Steady-State Conduction
Pharos University جامعه فاروس Faculty of Engineering كلية الهندسة Petrochemical Department قسم البتروكيماويات PE 330 ENERGY CONSERVATION LECTURES (6-7)
Heat Transfer Equations. Fouling Layers of dirt, particles, biological growth, etc. effect resistance to heat transfer We cannot predict fouling factors.
SELECTING INSULATION MATERIALS  Insulation can serve as more than just an energy barrier, providing fire resistance, humidity control, and noise reduction.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Solar Gain The ultimate free lunch!. Some Basics Why do we need to heat our homes? –Living rooms21 o C –Bedrooms18 o C –Staircases & halls16 o C.
Conservation of Building Energy 3A9 Construction Technology Dr S Pavía Dept of Civil Engineering Trinity College Dublin.
Exercises for Q1. Insulated copper tube A thin walled 10 mm copper tube is used to transport a low-temperature refrigerant with a temperature that is.
Heat loss, U-values and all that stuff. First a bit of Science First Law of Thermodynamics You can’t get more heat out of a closed system than you put.
TUTORIAL 1 7/3/2016.
HEAT TRANSFER Problems with FEM solution
Lesson 7: Thermal and Mechanical Element Math Models in Control Systems ET 438a Automatic Control Systems Technology 1lesson7et438a.pptx.
Heat transfer Steady state conditions not for dynamic systems in buildings through walls, roofs, floors, windows, doors building structures and U-values.
Under floor heating Designing underfloor heating (UFH) system must always comply with the system suppliers instructions.
Load Estimating Fundamentals
HEAT TRASNFER IN BUILDINGS
One-Dimensional Steady-State Conduction
Chapter 18. Heat Transfer A PowerPoint Presentation by
Conservation of Mass and Energy
RESIDENTIAL HVAC (HEAT LOSS & GAIN)
Thermal mass dynamics 1.00 Heat absorption
Building Energy Analysis
Insulating Houses.
Heat gain and heat loss in buildings
Heat and Mass Transfer Heat is ……… Heat Transfer ……
Heat Loss and Gain Heat Transfer Winter Heat Loss Summer Heat Gain
Conduction Cooling Loads
Chapter 8 : Natural Convection
Temperature, Heat, and the First Law of Thermodynamics
Temperature and Heat Loss
Heat Loss and Gain Heat Loss and Gain
Heat Exchangers Heat Exchangers.
Heat Loss and Gain Heat Loss and Gain
Chapter 18. Heat Transfer A PowerPoint Presentation by
Heat Loss and Gain Civil Engineering and Architecture
Temperature, Heat, and the First Law of Thermodynamics
Heat Loss and Gain Heat Loss and Gain
HEAT EXCHANGE IN BUILDINGS. TERMINOLOGIES Thermal conductivity: is the rate of heat flow through a unit area of unit thickness of the material for a unit.
Heat Loss and Gain Heat Loss and Gain
Presentation transcript:

THERMAL LOADING OF BUILDINGS U-value Thermal conductivity Temperature dependence Effects of Pressure and Density Effect of moisture content Cavity walls and other air gaps Factors affecting surface resistances Roofs Ground floors and basements Windows Effects of blinds and curtains Energy flows associated with ventilation and infiltration Natural ventilation Mechanical ventilation Heat transfer associated with ventilation

U-VALUE When selecting materials for construction, we choose good insulators to reduce heat energy losses. In practice, it is usual to use a figure for a particular structure, e.g. a brick wall, rather than take the values of the conductivities of its constituent materials. The figure used is called the U-value. It refers to Unit Heat Loss Rate , and its unit is the watt per metre squared per kelvin, W m-2 K-1. The U-value is defined as the rate at which thermal energy is conducted through unit area, per kelvin temperature difference between its two sides. U = rate of loss of energy/(surface area)(temperature difference) A good insulating structure therefore has a low U-value, if a structure has a U-value of 1, this means 1 J per second will pass through each square metre for each kelvin (degree Celsius) difference in temperature between the two sides of the structure. U-value is also referred to as an ‘overall heat transfer co-efficient’ and measures how well parts of a building transfer heat. This means that the higher the U-value the worse the thermal performance of the building envelope. A low U-value usually indicates high levels of insulation. They are useful as it is a way of predicting the composite behaviour of an entire building element rather than relying on the properties of individual materials.

IMPORTANCE OF U-VALUE U-values are important because they form the basis of any energy or carbon reduction standard. In practice, nearly every external building element has to comply with thermal standards that are expressed as a maximum U-value. Knowledge of how to simply calculate U-values at an early stage in the design process, avoids expensive re-working later on in a project. It allows the designer to test the feasibility of their project at an early stage to ensure it is fit for purpose and will comply with regulatory frameworks.

EFFECT OF INSULATION ON U-VALUES

U-VALUES OF WINDOWS

CALCULATION OF U-VALUE To calculate the U value of a building element such as a wall, floor or roof, you need to know the build up of that element. Each building material should be positioned properly in sequence. The thickness of each building material also is required. The other key property you need to obtain is the conductivity of each building material. This is a measure of its inherent ability to facilitate the passage of heat. It is normally referred to as a ‘k value’ and values for materials can be found in publications such as the New Metric Handbook and the Architects’ Pocket Guide The properties of the internal and external faces of the constructional element under scrutiny need to be allowed for. These are called external resistances and are fixed values. The U-value is defined as being reciprocal of all the resistances of the materials found in the building element. The resistance of a building material is derived by the following formula: R = (x/k) where k is the conductivity of the building material and x is the material thickness. The formula for the calculation of a U value is U(element) = 1 / (Rso + Rsi + R1 + R2 ...)

U-VALUE The reciprocal of the total thermal resistance of a body is regarded as the overall thermal transmittance or U-value. R = 1/U Q = kA(T1-T2)/x Q = A(T1-T2)/R Where R = thermal resistance = x/k or L/k Q =UA(T1-T2)

U-VALUE OF WINDOWS

U-VALUE OF WINDOWS

ONLINE U-VALUE CALCULATOR http://www.uvalue.co.uk/U-Value-Calculator Celotex insulation http://www.celotex.co.uk/Other-Resources/U-value-Calculator

EXAMPLE Determine the U-value for an external brick cavity wall consisting of 100mm brick outer leaf of thermal conductivity of 0.84W/mK; a 50mm unvented air gap; and a 100mm block inner leaf of thermal conductivity 0.17W/mK. The internal surface, external surface and air resistances are respectively 0.06, 0.12 and 0.18m2K/W 1/U = Ros+x1/k1+Ra+x2/k2+Ris 1/U = 0.12+0.1/0.84+0.18+0.1/0.17+0.06 = 1.06m2K/W U = 1/1.06 = 0.94W/m2K

EXAMPLE A cold-storage room has walls constructed of 0.23 m brick on the outside, 0.08 m of insulation foam, and finally 0.015 m of wood on the inside. The total wall area is 90 m2. The outdoor air temperature is constant at 22°C, and the air temperature inside is constant at -2°C. The convection coefficient from wood to air is 29 W/m2 K, and the convection coefficient from air to brick is 12 W/m2 K, and the thermal conductivities of wood, foam and brick are 0.17,0.024, and 0.98 W/m K respectively. It can be assumed that the heat transfer by radiation may be neglected. Determine: the overall heat transfer coefficient the energy to be removed by the refrigeration equipment in twenty four hours the temperature of the inner surface of the brick.

Solution The overall heat transfer coefficient is given by 1/U=R=1/ho+x1/k1+x2/k2+x3/k3+1/h1 1/U=1/12 +0.23/0.98+0.08/0.024+0.015/0.17+1/29 = 3.77m2K/W U=0.265W/m2K Q = UA∆T = 0.265 x 90 x [22-(-2)] = 572W E =24 x 572=13.7kWh Q = Ak3/x3 ∆T 572 = 90 x 0.98/0.23 (22-T) T=20.5C