<Dl> <Dd> See Density for a table of the measured densities of water at various temperatures . </Dd> </Dl> <Dd> See Density for a table of the measured densities of water at various temperatures . </Dd> <P> The density of substances varies with temperature and pressure so that it is necessary to specify the temperatures and pressures at which the densities or masses were determined . It is nearly always the case that measurements are made at nominally 1 atmosphere (101.325 kPa the variations caused by changing weather patterns) but as relative density usually refers to highly incompressible aqueous solutions or other incompressible substances (such as petroleum products) variations in density caused by pressure are usually neglected at least where apparent relative density is being measured . For true (in vacuo) relative density calculations air pressure must be considered (see below). Temperatures are specified by the notation T / T) with T representing the temperature at which the sample's density was determined and T the temperature at which the reference (water) density is specified . For example, SG (20 ° C / 4 ° C) would be understood to mean that the density of the sample was determined at 20 ° C and of the water at 4 ° C. Taking into account different sample and reference temperatures we note that while SG = 1.000000 (20 ° C / 20 ° C) it is also the case that RD = 0.998203 / 0.998840 = 0.998363 (20 ° C / 4 ° C). Here temperature is being specified using the current ITS - 90 scale and the densities used here and in the rest of this article are based on that scale . On the previous IPTS - 68 scale the densities at 20 ° C and 4 ° C are, respectively, 0.9982071 and 0.9999720 resulting in an RD (20 ° C / 4 ° C) value for water of 0.9982343 . </P> <P> The temperatures of the two materials may be explicitly stated in the density symbols; for example: </P>

What is the value of relative density of water