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Book - School of Science and Technology

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2 FundamentalsBefore any part <strong>of</strong> this subject is pursued in further detail, however, it would seemappropriate to discuss some <strong>of</strong> the quantities <strong>and</strong> units that are relevant, with particularreference to the meaning <strong>and</strong> use applied to them in the present context.Units <strong>and</strong> quantitiesThe notes included here are not intended to be a comprehensive glossary <strong>of</strong> termsincluded in the SysteÁme International d'UniteÂs but, rather, an aide meÂmoire covering thosewhich are specific to the subject matter <strong>of</strong> this book but are not necessarily in everydayuse. The four basic units are the kilogram (kg) for mass, the metre (m) for length, thesecond (s) for time <strong>and</strong> the kelvin (K) for thermodynamic temperature, all with theirmultiples <strong>and</strong> sub-multiples. From these, the following secondary units are derived:Force. The unit here is the newton (N), which is the force necessary to accelerate a mass<strong>of</strong> one kilogram to a velocity <strong>of</strong> one metre per second in one second, that is,1Nˆ 1 kg m/s 2 . When a mass <strong>of</strong> 1 kg is subjected to acceleration due to gravity, theforce then exerted is 9.81 N.Heat. The unit <strong>of</strong> energy, including heat energy, is the joule (J), which is equal to a force <strong>of</strong>one newton acting through one metre.Heat Flow. The rate <strong>of</strong> heat flow is represented by the watt (W), which is equal to onejoule produced or expended in one second, that is, 1 W ˆ 1 J/s ˆ 1 Nm/s.Pressure. The st<strong>and</strong>ard unit is the newton per square metre (N/m 2 ), also known, moreconveniently, as the pascal (Pa). The bar continues to be used in some circumstances<strong>and</strong> 1 bar ˆ 100 k Pa.Specific Heat Capacity. This is the quantity <strong>of</strong> heat required to raise the temperature <strong>of</strong>one kilogram <strong>of</strong> a substance through one kelvin, the units being kJ/kg K. Where heatflow in unit time is involved, the unit becomes kJ/s kg K ˆ kW/kg K.Specific Density. The unit for this quantity is the kilogram per cubic metre (kg/m 3 ).Volume. The cubic metre is the preferred unit but the litre (1 dm 3 ) is in general use since itis much more convenient in terms <strong>of</strong> a comprehensible size. To avoid printing confusionbetween the figure 1 <strong>and</strong> the letter l, this book will spell out the world litre in full.Properties <strong>of</strong> materialsTable 1.1 lists a variety <strong>of</strong> materials <strong>and</strong> provides details <strong>of</strong> some relevant physicalproperties. These serve as a source <strong>of</strong> reference against the following notes:Latent heat. When the temperature <strong>of</strong> water at atmospheric pressure, is raised fromfreezing to boiling point, i.e. through 100 C, the heat added is 420 kJ/kg (4:2 100). Toconvert this hot water to steam, however, still at atmospheric pressure <strong>and</strong> still at 100 C,will require the addition <strong>of</strong> a significantly greater quality <strong>of</strong> heat, i.e. 2257 kJ/kg.*This value is the latent heat <strong>of</strong> evaporation <strong>of</strong> water <strong>and</strong> its magnitude, 5.4 times thatneeded to raise water through 100 C shows its importance. A similar phenomenon occurswhen water at 0 C becomes ice at the same temperature; this change <strong>of</strong> state releasing330 kJ/kg, the latent heat <strong>of</strong> fusion <strong>of</strong> water.* If water is evaporated at 20 C, the latent heat <strong>of</strong> evaporation is 2450 kJ/kg.

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