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Medio Ambiente 13 2 : Helgoland Marine Research Catholic : Canadian Journal of Fisheries and Aquatic Sciences 63 5 : Life and Environment 56 3 : Journal of Great Lakes Research Western : This is then used to calculate the vapour pressure at a given temperature. In the spinning rotor gauge, the actual measuring element is a small steel ball which is suspended in a magnetic field and rotates with high speed. The gas pressure is deduced from the pressure-dependent slow-down of the steel ball.

The various methods of determining the vapour pressure are compared as to application, repeatability, reproducibility, measuring range, existing standard. This is done in the following table. The measuring apparatus typically consists of a boiling vessel with attached cooler made of glass or metal figure 1 , equipment for measuring the temperature, and equipment for regulating and measuring the pressure. A typical measuring apparatus shown in the drawing is made from heat-resistant glass and is composed of five parts:. The large, partially double-walled tube consists of a ground jacket joint, a cooler, a cooling vessel and an inlet.

The temperature is measured with a suitable temperature sensor e. The necessary connections are made to the pressure regulation and measuring equipment. The bulb, which acts as a buffer volume, is connected with the measuring apparatus by means of a capillary tube. The boiling vessel is heated by a heating element e.

The heating current required is set and regulated via a thermocouple. The necessary vacuum of between 10 2 Pa and approximately 10 5 Pa is produced with a vacuum pump. A suitable valve is used to meter air or nitrogen for pressure regulation measuring range approximately 10 2 to 10 5 Pa and ventilation.

BS 6401; ASTM E662; NFPA 258 Options: ISO 5659/IMO FTPC Part 2; ATS 1000.001/ABD0031; NES 711

The vapour pressure is measured by determining the boiling temperature of the sample at various specified pressures between roughly 10 3 and 10 5 Pa. A steady temperature under constant pressure indicates that the boiling temperature has been reached. Frothing substances cannot be measured using this method. The substance is placed in the clean, dry sample vessel.


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Problems may be encountered with non-powder solids but these can sometimes be solved by heating the cooling jacket. Once the vessel has been filled the apparatus is sealed at the flange and the substance degassed. The lowest desired pressure is then set and the heating is switched on. At the same time, the temperature sensor is connected to a recorder. Equilibrium is reached when a constant boiling temperature is recorded at constant pressure. Particular care must be taken to avoid bumping during boiling.

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In addition, complete condensation must occur on the cooler. When determining the vapour pressure of low melting solids, care should be taken to avoid the condenser blocking. After recording this equilibrium point, a higher pressure is set. The process is continued in this manner until 10 5 Pa has been reached approximately 5 to 10 measuring points in all.

As a check, equilibrium points must be repeated at decreasing pressures. The apparatus comprises a container for the sample, a heating and cooling system to regulate the temperature of the sample and measure the temperature. The apparatus also includes instruments to set and measure the pressure.

Test Laboratory

Figures 2a and 2b illustrate the basic principles involved. The sample chamber figure 2a is bounded on one side by a suitable high-vacuum valve. A U-tube containing a suitable manometer fluid is attached to the other side.


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One end of the U-tube branches off to the vacuum pump, the nitrogen cylinder or ventilation valve, and a manometer. A pressure gauge with a pressure indicator can be used instead of a U-tube figure 2b. The temperature measurements are taken on the outside wall of the vessel containing the sample or in the vessel itself.

In method 2a the vapour pressure of the substance is measured indirectly using a zero indicator. This takes into account the fact that the density of the fluid in the U-tube alters if the temperature changes greatly. The following fluids are suitable for use as zero indicators for the U-tube, depending on the pressure range and the chemical behaviour of the test substance: silicone fluids, phthalates. The test substance must not dissolve noticeably in or react with the U-tube fluid.

For the manometer, mercury can be used in the range of normal air pressure to 10 2 Pa, while silicone fluids and phthalates are suitable for use below 10 2 Pa down to 10 Pa. Heatable membrane capacity manometers can even be used at below 10 -1 Pa. There are also other pressure gauges which can be used below 10 2 Pa. Before measuring, all components of the apparatus shown in figure 2 must be cleaned and dried thoroughly. For method 2a, fill the U-tube with the chosen liquid, which must be degassed at an elevated temperature before readings are taken.

The test substance is placed in the apparatus, which is then closed and the temperature is reduced sufficiently for degassing. The temperature must be low enough to ensure that the air is sucked out, but — in the case of multiple component system — it must not alter the composition of the material. If required, equilibrium can be established more quickly by stirring. The sample can be supercooled with e. For low-temperature measurements use a temperature-regulated bath connected to an ultra-cryomat. With the valve over the sample vessel open, suction is applied for several minutes to remove the air.

The valve is then closed and the temperature of the sample reduced to the lowest level desired. If necessary, the degassing operation must be repeated several times. When the sample is heated the vapour pressure increases.

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Interlaboratory Evaluation of Smoke Density Chamber (Classic Reprint) by T G Lee - atconlaroreal.gq

This alters the equilibrium of the fluid in the U-tube. To compensate for this, nitrogen or air is admitted to the apparatus via a valve until the pressure indicator fluid is at zero again. The pressure required for this can be read off a precision manometer at room temperature. This pressure corresponds to the vapour pressure of the substance at that particular measuring temperature.

The temperature-dependence of vapour pressure is determined at suitably small intervals approximately 5 to 10 measuring points in all up to the desired maximum. Low-temperature readings must be repeated as a check. If the values obtained from the repeated readings do not coincide with the curve obtained for increasing temperature, this may be due to one of the following:. In this case liquid nitrogen is used as the cooling agent.

A complete description of this method can be found in reference 7. The principle of the measuring device is shown in figure 3. Similarly to the static method described in 1. In the case of liquids, the substance itself serves as the fluid in the auxiliary manometer.

A quantity of the liquid, sufficient to fill the bulb and the short leg of the manometer section, is put in the isoteniscope. The isoteniscope is attached to a vacuum system and evacuated, then filled by nitrogen. The evacuation and purge of the system is repeated twice to remove residual oxygen.

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