CA2153286C - Apparatus for measuring surface tension - Google Patents
Apparatus for measuring surface tension Download PDFInfo
- Publication number
- CA2153286C CA2153286C CA002153286A CA2153286A CA2153286C CA 2153286 C CA2153286 C CA 2153286C CA 002153286 A CA002153286 A CA 002153286A CA 2153286 A CA2153286 A CA 2153286A CA 2153286 C CA2153286 C CA 2153286C
- Authority
- CA
- Canada
- Prior art keywords
- crucible
- capillary
- gas
- nozzle
- capillary tube
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 238000005259 measurement Methods 0.000 claims abstract description 22
- 239000000463 material Substances 0.000 claims description 4
- 239000010453 quartz Substances 0.000 claims description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 3
- 239000012530 fluid Substances 0.000 claims 6
- PNEYBMLMFCGWSK-UHFFFAOYSA-N Alumina Chemical compound [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 claims 3
- RVTZCBVAJQQJTK-UHFFFAOYSA-N oxygen(2-);zirconium(4+) Chemical compound [O-2].[O-2].[Zr+4] RVTZCBVAJQQJTK-UHFFFAOYSA-N 0.000 claims 1
- 229910001928 zirconium oxide Inorganic materials 0.000 claims 1
- 239000007788 liquid Substances 0.000 abstract description 29
- 238000004519 manufacturing process Methods 0.000 abstract description 3
- 239000007789 gas Substances 0.000 description 45
- 229910001018 Cast iron Inorganic materials 0.000 description 16
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 9
- 239000000155 melt Substances 0.000 description 9
- 230000015572 biosynthetic process Effects 0.000 description 8
- 229910002804 graphite Inorganic materials 0.000 description 8
- 239000010439 graphite Substances 0.000 description 8
- 229910052751 metal Inorganic materials 0.000 description 5
- 239000002184 metal Substances 0.000 description 5
- 229910000805 Pig iron Inorganic materials 0.000 description 4
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 description 4
- 230000009286 beneficial effect Effects 0.000 description 4
- 150000002739 metals Chemical class 0.000 description 4
- 229910052684 Cerium Inorganic materials 0.000 description 3
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 description 3
- GWXLDORMOJMVQZ-UHFFFAOYSA-N cerium Chemical compound [Ce] GWXLDORMOJMVQZ-UHFFFAOYSA-N 0.000 description 3
- 229910052749 magnesium Inorganic materials 0.000 description 3
- 239000011777 magnesium Substances 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 229910000676 Si alloy Inorganic materials 0.000 description 2
- CSDREXVUYHZDNP-UHFFFAOYSA-N alumanylidynesilicon Chemical compound [Al].[Si] CSDREXVUYHZDNP-UHFFFAOYSA-N 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 238000009826 distribution Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000003801 milling Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 2
- 238000005070 sampling Methods 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- NINIDFKCEFEMDL-UHFFFAOYSA-N Sulfur Chemical compound [S] NINIDFKCEFEMDL-UHFFFAOYSA-N 0.000 description 1
- 239000005864 Sulphur Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 238000009530 blood pressure measurement Methods 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 239000004568 cement Substances 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 239000003779 heat-resistant material Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 235000000396 iron Nutrition 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 239000011819 refractory material Substances 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- 238000007711 solidification Methods 0.000 description 1
- 230000008023 solidification Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01L—CHEMICAL OR PHYSICAL LABORATORY APPARATUS FOR GENERAL USE
- B01L3/00—Containers or dishes for laboratory use, e.g. laboratory glassware; Droppers
- B01L3/04—Crucibles
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N13/00—Investigating surface or boundary effects, e.g. wetting power; Investigating diffusion effects; Analysing materials by determining surface, boundary, or diffusion effects
- G01N13/02—Investigating surface tension of liquids
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N13/00—Investigating surface or boundary effects, e.g. wetting power; Investigating diffusion effects; Analysing materials by determining surface, boundary, or diffusion effects
- G01N13/02—Investigating surface tension of liquids
- G01N2013/0225—Investigating surface tension of liquids of liquid metals or solder
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N13/00—Investigating surface or boundary effects, e.g. wetting power; Investigating diffusion effects; Analysing materials by determining surface, boundary, or diffusion effects
- G01N13/02—Investigating surface tension of liquids
- G01N2013/0241—Investigating surface tension of liquids bubble, pendant drop, sessile drop methods
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N13/00—Investigating surface or boundary effects, e.g. wetting power; Investigating diffusion effects; Analysing materials by determining surface, boundary, or diffusion effects
- G01N13/02—Investigating surface tension of liquids
- G01N2013/0241—Investigating surface tension of liquids bubble, pendant drop, sessile drop methods
- G01N2013/0266—Bubble methods
Landscapes
- Chemical & Material Sciences (AREA)
- Health & Medical Sciences (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Clinical Laboratory Science (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Measuring Fluid Pressure (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Investigating Or Analyzing Materials Using Thermal Means (AREA)
- Sampling And Sample Adjustment (AREA)
Abstract
An apparatus for the measurement of the surface tension of liquids by means of a capillary tube for supplying gas, the tube having a connector and a nozzle, may be used in a measuring device. In order to create an apparatus that is easy to manufacture and handle, and that can be used reliably in a variety of liquids, the capillary tube is arranged, at least partially, in a crucible for receiving the liquid and is mounted on the wall of the crucible, whereby the connector is arranged outside the interior of the crucible. The connector is connected to the gas line of the measuring device and to a pressure sensor and/or a flow meter.
Description
.i Attorney Docket No. 925-241 APPARATUS FOR MEASURING SURFACE TENSION
Field of the Invention The invention pertains to an apparatus for measurement of the surface tension of liquids by means of a capillary tube for supplying gas, which has a connector and a nozzle, wherein the capillary tube is at least partially arranged in a crucible for receiving the liquid and wherein the connector is arranged outside the interior of the crucible. The invention also pertains to a measuring device with an apparatus of this type.
Background Of The Invention An apparatus of this type is known from DE 22 31 598/A1, in which an apparatus and process are disclosed for determining the surface tension at the interface between liquids and gases. The apparatus uses a capillary tube for supplying gas with a connector and a nozzle. The capillary tube extends from above down into the container which receives the liquid. For measurement in molten metals the capillary tube is exposed to the heat which rises from the liquid to be measured. The capillary tube is mounted outside of the crucible. Such an arrangement is rather expensive.
A further apparatus of this type is known from DE 29 15 956/A1, in which is described an apparatus for measuring the surface tension of electrically conductive liquids. This apparatus has a capillary tube with a connecting sleeve and a nozzle. The end of the capillary tube that carries the nozzle is bent in a U-shape. The capillary tube is immersed from above in a liquid so that the nozzle is pointing in an upward direction. During operation of the apparatus, gas bubbles exit the nozzle and rise vertically inside a measuring tube.
Two electrodes supplied with a voltage and connected to a time-keeping device are arranged on the measuring tube. When the gas bubbles pass between the electrodes, an interruption in the current flowing between the electrodes is brought about; the frequency of the interruptions that the gas bubbles cause in the electrical circuit is measured. The capillary tube is supplied with a flow of gas at a constant pressure, so that by making use of the frequency of the gas bubbles, the surface tension of the liquid can be determined.
Apparatus of this type are relatively complicated, since the capillary tube immersed in the liquid from above must be additionally mounted, like the measuring tube that has the electrodes. In conjunction with that, these elements must at the same time be protected from the increasing heat from molten metals, for example. Even the necessity for generating a flow of current within the liquid requires a relatively high expenditure for operation and safety. The danger of possible leaking currents also has to be viewed as a problem, if the gas bubbles do not perfectly insulate the electrodes from one another, since the results of the measurement can be distorted as a result of such current leaks.
Further, an apparatus is known from DE 42 28 942/Cl for measurement of the surface tension in liquids, wherein a capillary tube is partially arranged in a crucible for receiving the liquid, and wherein the capillary tube extends through the wall of the crucible. The gas to be conducted into the liquid flows through the capillary tube by way of a gas distribution unit. The gas flows out over the entire surface of the gas distribution unit, more or less irregularly, and thereby reaches the surface of the liquid under constantly changing conditions, where a sampling device catches a portion of the gas bubbles (as a rule the largest) and Ieads these as a measuring impulse to an analysis. Due to the different outlet openings, the different paths of the gas bubbles to the liquid, and due to the different size gas bubbles emitted by the distributing unit, as well as due to the inexactness of the receiving of the sampling device arranged over the liquid, an exact measurement of the surface tension with the described apparatus is not possible, since 2153~~6 such an apparatus as a rule will not completely and correctly catch the gas bubbles which escape from the liquid at different places and in different sizes.
An additional apparatus for measurement of surface tensions is described in EP 0 149 500. Also, the determination of the frequency of gas bubbles, here in liquid pig iron, is described in G.A. Irons and R.I.C. Guthrie "Bubble Formation at Nozzles in Pig Iron," Metallurgical Transactions B, Volume 9B, pages 101 - 110, March 1978. Shown here is an apparatus in which the gas bubbles are detected by means of a microphone.
By making use of the surface tension, apparatus of this type are used, by way of example, to determine the properties of molten metals. Knowledge of the surface tension of molten cast iron makes it possible, among other things, to draw conclusions concerning the graphite morphology of the carbon contained in the cast iron, since the surface tension and the interfacial energy between various phases influence the microstructure of an alloy. This effect is described in the article by E. Selcuk and D. H. Kirkwood, "Surface Energies of Liquid Cast Irons Containing Magnesium and Cerium", Journal of the Iron and Steel Institute, pages 134 - 140, February 1973. Admixtures of cerium and magnesium with cast iron accelerate the formation of spheroidal graphite, that is, with increasing content of cerium or magnesium, the form of the graphite crystals changes from the lamellar type of graphite at the beginning to the spheroidal type (spheroidal graphite), which is sought in the practice of casting, because a graphite morphology of this type generates optimal strength properties in the cast iron.
Summary of the Invention Building on the present state of the art described above, it is an object of the present invention to create an apparatus that is easy to manufacture and handle, and that can be used reliably in a variety of liquids. For an apparatus of the above type, this object is achieved by means of the capillary tube being arranged, at least partially, in a crucible for receiving and holding the liquid and being mounted on a wall of the crucible, whereby the connector is arranged outside the interior of the crucible. An apparatus of this type is relatively simple to manufacture and ensures a secure placement of the capillary tube within the liquid with which the crucible is to be filled, without the danger that heat rising from a liquid that might be very hot, such as molten metals, could damage the mount or the measurement device, since no delicate parts need be placed above the liquid. An apparatus of this type is suitable for measuring the surface tensions of a variety of liquids, even for measurements in liquid cast iron in order to determine, among other things, the graphite morphology; for the determination of the sulphur content of pig iron; or in order to assess the modification treatment of aluminum-silicon alloys.
It is beneficial that the capillary tube be run through the wall of the crucible, particularly through the bottom of the crucible, in order to ensure a secure mounting.
When it is arranged in the bottom, the capillary tube can be aligned vertically so that the gas bubbles can exit the capillary tube unrestrictedly and in accordance with their buoyancy. Additionally, it is beneficial if the connector is mounted on or in the bottom of the crucible and is configured as a crucible mounting, since the crucible can then be placed with the connector directly on the gas connecting sleeve of a gas supply line, and does not need to be fastened by additional means.
For the uniform formation of bubbles it is advantageous that the inside diameter of the capillary tube increases at the nozzle and, in particular, is increased in a circular manner or, that the nozzle is expanded in a slit-like shape. In conjunction with this, it is beneficial that the difference between the inside and the outside diameters of the capillary tube at the outer end of the nozzle not be greater 2I~3286 than 1 mm, and particularly not greater than 0.5 mm, and/or that the product of the thermal conductivity (W/K-m) and the wall thickness of the capillary tube at the outer end of the nozzle be smaller than 5.5 x 10-3 W/K (Watt/Kelvin) at 1400°C.
An arrangement of this type ensures the regular formation of bubbles that always exhibit a practically uniform diameter.
It is also possible for the nozzle to be placed laterally on the capillary tube, by means of a lateral bore or a slit that is made (by means of sawing or milling, for example) in the capillary tube, for example.
It is advantageous, particularly for measurements in aggressive or very hot media, that the capillary tube be made of a gas-tight material, such as aluminum oxide, quartz, or zirconia, since these materials exhibit high temperature stability and are chemically resistant to many media, such as cast iron melts. For the accuracy and reproducability of measurements it is beneficial that the connector be joined to the crucible in a gas-tight manner.
For a measurement device, the object is achieved by virtue of the fact that the connector is connected in a gas-tight manner to a gas connecting sleeve of a gas line and to a pressure sensor and/or flow meter, since the frequency of the gas bubbles that appear can be measured by using these devices.
Brief Description of the Drav~ings The foregoing summary, as well as the following detailed description of preferred embodiments of the invention, will be better understood when read in conjunction with the appended drawings which show further features and advantages of the invention. For the purpose of illustrating the invention, there are shown in the drawings embodiments which are presently preferred. It should be understood, however, that the invention is not limited to the precise arrangements and instrumentalities shown. In the drawings:
21~328~
Field of the Invention The invention pertains to an apparatus for measurement of the surface tension of liquids by means of a capillary tube for supplying gas, which has a connector and a nozzle, wherein the capillary tube is at least partially arranged in a crucible for receiving the liquid and wherein the connector is arranged outside the interior of the crucible. The invention also pertains to a measuring device with an apparatus of this type.
Background Of The Invention An apparatus of this type is known from DE 22 31 598/A1, in which an apparatus and process are disclosed for determining the surface tension at the interface between liquids and gases. The apparatus uses a capillary tube for supplying gas with a connector and a nozzle. The capillary tube extends from above down into the container which receives the liquid. For measurement in molten metals the capillary tube is exposed to the heat which rises from the liquid to be measured. The capillary tube is mounted outside of the crucible. Such an arrangement is rather expensive.
A further apparatus of this type is known from DE 29 15 956/A1, in which is described an apparatus for measuring the surface tension of electrically conductive liquids. This apparatus has a capillary tube with a connecting sleeve and a nozzle. The end of the capillary tube that carries the nozzle is bent in a U-shape. The capillary tube is immersed from above in a liquid so that the nozzle is pointing in an upward direction. During operation of the apparatus, gas bubbles exit the nozzle and rise vertically inside a measuring tube.
Two electrodes supplied with a voltage and connected to a time-keeping device are arranged on the measuring tube. When the gas bubbles pass between the electrodes, an interruption in the current flowing between the electrodes is brought about; the frequency of the interruptions that the gas bubbles cause in the electrical circuit is measured. The capillary tube is supplied with a flow of gas at a constant pressure, so that by making use of the frequency of the gas bubbles, the surface tension of the liquid can be determined.
Apparatus of this type are relatively complicated, since the capillary tube immersed in the liquid from above must be additionally mounted, like the measuring tube that has the electrodes. In conjunction with that, these elements must at the same time be protected from the increasing heat from molten metals, for example. Even the necessity for generating a flow of current within the liquid requires a relatively high expenditure for operation and safety. The danger of possible leaking currents also has to be viewed as a problem, if the gas bubbles do not perfectly insulate the electrodes from one another, since the results of the measurement can be distorted as a result of such current leaks.
Further, an apparatus is known from DE 42 28 942/Cl for measurement of the surface tension in liquids, wherein a capillary tube is partially arranged in a crucible for receiving the liquid, and wherein the capillary tube extends through the wall of the crucible. The gas to be conducted into the liquid flows through the capillary tube by way of a gas distribution unit. The gas flows out over the entire surface of the gas distribution unit, more or less irregularly, and thereby reaches the surface of the liquid under constantly changing conditions, where a sampling device catches a portion of the gas bubbles (as a rule the largest) and Ieads these as a measuring impulse to an analysis. Due to the different outlet openings, the different paths of the gas bubbles to the liquid, and due to the different size gas bubbles emitted by the distributing unit, as well as due to the inexactness of the receiving of the sampling device arranged over the liquid, an exact measurement of the surface tension with the described apparatus is not possible, since 2153~~6 such an apparatus as a rule will not completely and correctly catch the gas bubbles which escape from the liquid at different places and in different sizes.
An additional apparatus for measurement of surface tensions is described in EP 0 149 500. Also, the determination of the frequency of gas bubbles, here in liquid pig iron, is described in G.A. Irons and R.I.C. Guthrie "Bubble Formation at Nozzles in Pig Iron," Metallurgical Transactions B, Volume 9B, pages 101 - 110, March 1978. Shown here is an apparatus in which the gas bubbles are detected by means of a microphone.
By making use of the surface tension, apparatus of this type are used, by way of example, to determine the properties of molten metals. Knowledge of the surface tension of molten cast iron makes it possible, among other things, to draw conclusions concerning the graphite morphology of the carbon contained in the cast iron, since the surface tension and the interfacial energy between various phases influence the microstructure of an alloy. This effect is described in the article by E. Selcuk and D. H. Kirkwood, "Surface Energies of Liquid Cast Irons Containing Magnesium and Cerium", Journal of the Iron and Steel Institute, pages 134 - 140, February 1973. Admixtures of cerium and magnesium with cast iron accelerate the formation of spheroidal graphite, that is, with increasing content of cerium or magnesium, the form of the graphite crystals changes from the lamellar type of graphite at the beginning to the spheroidal type (spheroidal graphite), which is sought in the practice of casting, because a graphite morphology of this type generates optimal strength properties in the cast iron.
Summary of the Invention Building on the present state of the art described above, it is an object of the present invention to create an apparatus that is easy to manufacture and handle, and that can be used reliably in a variety of liquids. For an apparatus of the above type, this object is achieved by means of the capillary tube being arranged, at least partially, in a crucible for receiving and holding the liquid and being mounted on a wall of the crucible, whereby the connector is arranged outside the interior of the crucible. An apparatus of this type is relatively simple to manufacture and ensures a secure placement of the capillary tube within the liquid with which the crucible is to be filled, without the danger that heat rising from a liquid that might be very hot, such as molten metals, could damage the mount or the measurement device, since no delicate parts need be placed above the liquid. An apparatus of this type is suitable for measuring the surface tensions of a variety of liquids, even for measurements in liquid cast iron in order to determine, among other things, the graphite morphology; for the determination of the sulphur content of pig iron; or in order to assess the modification treatment of aluminum-silicon alloys.
It is beneficial that the capillary tube be run through the wall of the crucible, particularly through the bottom of the crucible, in order to ensure a secure mounting.
When it is arranged in the bottom, the capillary tube can be aligned vertically so that the gas bubbles can exit the capillary tube unrestrictedly and in accordance with their buoyancy. Additionally, it is beneficial if the connector is mounted on or in the bottom of the crucible and is configured as a crucible mounting, since the crucible can then be placed with the connector directly on the gas connecting sleeve of a gas supply line, and does not need to be fastened by additional means.
For the uniform formation of bubbles it is advantageous that the inside diameter of the capillary tube increases at the nozzle and, in particular, is increased in a circular manner or, that the nozzle is expanded in a slit-like shape. In conjunction with this, it is beneficial that the difference between the inside and the outside diameters of the capillary tube at the outer end of the nozzle not be greater 2I~3286 than 1 mm, and particularly not greater than 0.5 mm, and/or that the product of the thermal conductivity (W/K-m) and the wall thickness of the capillary tube at the outer end of the nozzle be smaller than 5.5 x 10-3 W/K (Watt/Kelvin) at 1400°C.
An arrangement of this type ensures the regular formation of bubbles that always exhibit a practically uniform diameter.
It is also possible for the nozzle to be placed laterally on the capillary tube, by means of a lateral bore or a slit that is made (by means of sawing or milling, for example) in the capillary tube, for example.
It is advantageous, particularly for measurements in aggressive or very hot media, that the capillary tube be made of a gas-tight material, such as aluminum oxide, quartz, or zirconia, since these materials exhibit high temperature stability and are chemically resistant to many media, such as cast iron melts. For the accuracy and reproducability of measurements it is beneficial that the connector be joined to the crucible in a gas-tight manner.
For a measurement device, the object is achieved by virtue of the fact that the connector is connected in a gas-tight manner to a gas connecting sleeve of a gas line and to a pressure sensor and/or flow meter, since the frequency of the gas bubbles that appear can be measured by using these devices.
Brief Description of the Drav~ings The foregoing summary, as well as the following detailed description of preferred embodiments of the invention, will be better understood when read in conjunction with the appended drawings which show further features and advantages of the invention. For the purpose of illustrating the invention, there are shown in the drawings embodiments which are presently preferred. It should be understood, however, that the invention is not limited to the precise arrangements and instrumentalities shown. In the drawings:
21~328~
Fig. 1 is a sectional side view of a schematic representation of an apparatus in accordance with the invention, with arrangement of the capillary tube in the bottom of the crucible;
Fig. 2 is a sectional side view of a schematic representation of the apparatus with arrangement of the capillary tube in a side wall of the crucible;
Figs. 3a-h are longitudinal section views of several forms of nozzles for the capillary tube;
Fig. 4 is a schematic representation, partially in section, of a measuring device incorporating the apparatus of the invention;
Fig. 5 is a pressure measurement curve for determination of the bubble frequency;
Fig. 6 is a sectional side view of a schematic representation of an apparatus similar to Fig. 1, but with the nozzle formed as a slit-like opening laterally on the capillary tube; and Fig. 7 is a sectional side view of a schematic representation of an apparatus similar to Fig. 2, but with the nozzle formed as a slit-like opening laterally on the capillary tube.
Detailed Description of Preferred Embodiment The crucible 1 shown in Fig. 1 is used for measurement of the surface tension of cast iron melts.
However, it is also suitable for measurements of aluminum-silicon alloys or pig iron, for example. The crucible is made of a heat-resistant material, in the present case of resin-bonded sand or ceramic fibers. The bottom of the crucible 1 is made stronger (thicker) than the side walls in order to ensure the necessary stability of the crucible. The capillary tube 2 is run all the way through the bottom of the crucible and is fastened there by means of a refractory cement 3 in such a way as to prevent the melt from running out through the bottom of the crucible.
_ 7 _ The capillary tube 2 is bonded to a connector 4, on which a gas connecting sleeve 5 is arranged. The connector 4 and the gas connecting sleeve 5 are used to supply gas to the capillary tube 2. The gas-tightness necessary for reproducability of measurements is ensured by means of two O-rings 6, which are arranged between the connector 4 and the gas connecting sleeve 5. The crucible 1 is connected to the gas supply line and the measuring device by means of the gas connecting sleeve 5. The connector 4 and gas connecting sleeve 5 are made of metal, and the capillary tube 2 is made of a refractory material, such as aluminum oxide, zirconia, or quartz, for example. The capillary tube has an inside diameter of about 0.7 - 1.5 mm and projects to a height of about 5 - 25 mm into the interior hollow area of the crucible 1 that holds the melt.
The hollow area of the crucible 1 holds a melt volume of about 100 ml; smaller volumes can lead to a cooling of the melt, starting at the crucible wall, that progresses too quickly to allow an accurate measurement of the surface tension of the melt, after the melt is poured into the crucible 1, since a volume that is too small has a correspondingly low heat capacity and, therefore, cools off correspondingly quickly. To minimize the influence of this cooling effect on the measurement, the capillary tube 2 is arranged approximately on the axis of the rotationally symmetrical crucible 1, and the nozzle 7 is located about in the middle of the hollow area of the crucible 1.
The crucible 1 shown in Fig. 2 is designed in a similar manner. The essential difference, with respect to the arrangement described above, resides in the arrangement of the capillary tube 2 in a side wall of the crucible 1.
Fig. 3 shows various nozzle forms for the capillary tube 2, as they can be used in the apparatus described at the beginning. What these nozzle forms have in common is that they are dimensioned in the apparatus in such a way that the difference between the outside and inside diameters of the . w 21~32$~
_8_ capillary tube at the outer end of the nozzle amounts to 0.5 mm at most, so that the formation of gas bubbles of uniform size is assured. In this regard, it is conceivable to keep the inside diameter of the capillary tube constant over the entire length of the capillary tube, and to dimension the outside diameter at the outer end of the nozzle in an appropriate manner, as is shown in Figs. 3 a, g, and h.
However, it is also conceivable to expand the inside diameter of the capillary tube at the nozzle in an appropriate manner.
In this regard, the expansion can be carried out in the form of a cylindrical enlargement of the diameter, as shown in Figs. 3 b and d, or as a conical expansion in the direction of the outer end of the nozzle, as shown in Figs. 3 c and f. A
combination of the two latter nozzle shapes is shown in Fig. 3 e; here, the inside diameter of the capillary tube is expanded in a cylindrical fashion, and an additional, conical expansion is joined only at the outer end of the nozzle.
A measuring device for the determination of surface tension is schematically shown in Fig. 4. The crucible 1 containing a cast iron melt 8 is connected to a gas line 9 through which the measurement gas is fed to the cast iron melt 8. The necessary gas flow is controlled by means of a gas flow regulating device 10 in the gas line 9. A gas that is inert with respect to the melt, such as argon or nitrogen, is used as the measurement gas that is blown into the cast iron melt 8 at about 2 - 15 ml per minute. The gas bubbles 11 are formed in the cast iron melt at the nozzle 7. In conjunction with this, a pressure that decreases abruptly following the release of the gas bubbles 11 from the nozzle 7 is built up in the gas line 9, and increases during the formation of a new gas bubble 11 until this bubble 11 releases.
This pressure sequence, which is shown as a function of time in Fig. 5, is detected and recorded by a pressure sensor 12. The frequency of these pressure fluctuations brought about by the formation of the gas bubbles 11 is used for the calculation of the surface tension of the cast iron _ g _ melt 8, or of a physical quantity that stands in a direct relationship with the surface tension, so that, as described at the beginning, the graphite morphology in the cast iron melt 8 can be determined. In this regard, the measurement time that is available for recording the pressure-time function is limited as a result of the solidification of the cast iron in the crucible 1. The available measurement time is determined by the difference between the pouring temperature of the cast iron melt 8 into the crucible 1 and the liquidus temperature of the cast iron, among other things.
In order to monitor the temperature, a temperature sensor such as a thermocouple, for example, can be placed in the hollow area of the crucible 1.
Figs. 6 and 7 illustrate further preferred embodiments, similar to Figs. 1 and 2, where the capillary tube 2 extends through the bottom or side wall, respectively, of the crucible. However, unlike Figs. 1 and 2, where the capillary tube opening or nozzle is formed in the end of the tube, for example-in one of the forms shown in Fig. 3, the nozzle 7 in Figs. 6 and 7 is in the form of a circumferential slit or slit-like opening the lateral wall of the capillary tube, preferably near its end inside the crucible and remote from the crucible bottom or side wall. This slit may suitably be formed by sawing or milling the tube in a radial or near radial direction, preferably perpendicular to the longitudinal axis of the tube. In the case of side wall mounting, the slit preferably faces upward to ensure free release and uniform bubble formation.
It will be appreciated by those skilled in the art that changes could be made to the embodiments described above without departing from the broad inventive concept thereof.
It is understood, therefore, that this invention is not limited to the particular embodiments disclosed, but it is intended to cover modifications within the spirit and scope of the present invention as defined by the appended claims.
Fig. 2 is a sectional side view of a schematic representation of the apparatus with arrangement of the capillary tube in a side wall of the crucible;
Figs. 3a-h are longitudinal section views of several forms of nozzles for the capillary tube;
Fig. 4 is a schematic representation, partially in section, of a measuring device incorporating the apparatus of the invention;
Fig. 5 is a pressure measurement curve for determination of the bubble frequency;
Fig. 6 is a sectional side view of a schematic representation of an apparatus similar to Fig. 1, but with the nozzle formed as a slit-like opening laterally on the capillary tube; and Fig. 7 is a sectional side view of a schematic representation of an apparatus similar to Fig. 2, but with the nozzle formed as a slit-like opening laterally on the capillary tube.
Detailed Description of Preferred Embodiment The crucible 1 shown in Fig. 1 is used for measurement of the surface tension of cast iron melts.
However, it is also suitable for measurements of aluminum-silicon alloys or pig iron, for example. The crucible is made of a heat-resistant material, in the present case of resin-bonded sand or ceramic fibers. The bottom of the crucible 1 is made stronger (thicker) than the side walls in order to ensure the necessary stability of the crucible. The capillary tube 2 is run all the way through the bottom of the crucible and is fastened there by means of a refractory cement 3 in such a way as to prevent the melt from running out through the bottom of the crucible.
_ 7 _ The capillary tube 2 is bonded to a connector 4, on which a gas connecting sleeve 5 is arranged. The connector 4 and the gas connecting sleeve 5 are used to supply gas to the capillary tube 2. The gas-tightness necessary for reproducability of measurements is ensured by means of two O-rings 6, which are arranged between the connector 4 and the gas connecting sleeve 5. The crucible 1 is connected to the gas supply line and the measuring device by means of the gas connecting sleeve 5. The connector 4 and gas connecting sleeve 5 are made of metal, and the capillary tube 2 is made of a refractory material, such as aluminum oxide, zirconia, or quartz, for example. The capillary tube has an inside diameter of about 0.7 - 1.5 mm and projects to a height of about 5 - 25 mm into the interior hollow area of the crucible 1 that holds the melt.
The hollow area of the crucible 1 holds a melt volume of about 100 ml; smaller volumes can lead to a cooling of the melt, starting at the crucible wall, that progresses too quickly to allow an accurate measurement of the surface tension of the melt, after the melt is poured into the crucible 1, since a volume that is too small has a correspondingly low heat capacity and, therefore, cools off correspondingly quickly. To minimize the influence of this cooling effect on the measurement, the capillary tube 2 is arranged approximately on the axis of the rotationally symmetrical crucible 1, and the nozzle 7 is located about in the middle of the hollow area of the crucible 1.
The crucible 1 shown in Fig. 2 is designed in a similar manner. The essential difference, with respect to the arrangement described above, resides in the arrangement of the capillary tube 2 in a side wall of the crucible 1.
Fig. 3 shows various nozzle forms for the capillary tube 2, as they can be used in the apparatus described at the beginning. What these nozzle forms have in common is that they are dimensioned in the apparatus in such a way that the difference between the outside and inside diameters of the . w 21~32$~
_8_ capillary tube at the outer end of the nozzle amounts to 0.5 mm at most, so that the formation of gas bubbles of uniform size is assured. In this regard, it is conceivable to keep the inside diameter of the capillary tube constant over the entire length of the capillary tube, and to dimension the outside diameter at the outer end of the nozzle in an appropriate manner, as is shown in Figs. 3 a, g, and h.
However, it is also conceivable to expand the inside diameter of the capillary tube at the nozzle in an appropriate manner.
In this regard, the expansion can be carried out in the form of a cylindrical enlargement of the diameter, as shown in Figs. 3 b and d, or as a conical expansion in the direction of the outer end of the nozzle, as shown in Figs. 3 c and f. A
combination of the two latter nozzle shapes is shown in Fig. 3 e; here, the inside diameter of the capillary tube is expanded in a cylindrical fashion, and an additional, conical expansion is joined only at the outer end of the nozzle.
A measuring device for the determination of surface tension is schematically shown in Fig. 4. The crucible 1 containing a cast iron melt 8 is connected to a gas line 9 through which the measurement gas is fed to the cast iron melt 8. The necessary gas flow is controlled by means of a gas flow regulating device 10 in the gas line 9. A gas that is inert with respect to the melt, such as argon or nitrogen, is used as the measurement gas that is blown into the cast iron melt 8 at about 2 - 15 ml per minute. The gas bubbles 11 are formed in the cast iron melt at the nozzle 7. In conjunction with this, a pressure that decreases abruptly following the release of the gas bubbles 11 from the nozzle 7 is built up in the gas line 9, and increases during the formation of a new gas bubble 11 until this bubble 11 releases.
This pressure sequence, which is shown as a function of time in Fig. 5, is detected and recorded by a pressure sensor 12. The frequency of these pressure fluctuations brought about by the formation of the gas bubbles 11 is used for the calculation of the surface tension of the cast iron _ g _ melt 8, or of a physical quantity that stands in a direct relationship with the surface tension, so that, as described at the beginning, the graphite morphology in the cast iron melt 8 can be determined. In this regard, the measurement time that is available for recording the pressure-time function is limited as a result of the solidification of the cast iron in the crucible 1. The available measurement time is determined by the difference between the pouring temperature of the cast iron melt 8 into the crucible 1 and the liquidus temperature of the cast iron, among other things.
In order to monitor the temperature, a temperature sensor such as a thermocouple, for example, can be placed in the hollow area of the crucible 1.
Figs. 6 and 7 illustrate further preferred embodiments, similar to Figs. 1 and 2, where the capillary tube 2 extends through the bottom or side wall, respectively, of the crucible. However, unlike Figs. 1 and 2, where the capillary tube opening or nozzle is formed in the end of the tube, for example-in one of the forms shown in Fig. 3, the nozzle 7 in Figs. 6 and 7 is in the form of a circumferential slit or slit-like opening the lateral wall of the capillary tube, preferably near its end inside the crucible and remote from the crucible bottom or side wall. This slit may suitably be formed by sawing or milling the tube in a radial or near radial direction, preferably perpendicular to the longitudinal axis of the tube. In the case of side wall mounting, the slit preferably faces upward to ensure free release and uniform bubble formation.
It will be appreciated by those skilled in the art that changes could be made to the embodiments described above without departing from the broad inventive concept thereof.
It is understood, therefore, that this invention is not limited to the particular embodiments disclosed, but it is intended to cover modifications within the spirit and scope of the present invention as defined by the appended claims.
Claims (12)
1. An apparatus for the measurement of the surface tension of fluids with a capillary for a gas supply, the capillary having a contact piece and a nozzle, in which the capillary is arranged at least partially in a crucible to receive the fluid and in which the contact piece is arranged outside the interior of the crucible, characterized in that the capillary is guided through a wall of the crucible and is mounted on the wall of the crucible and that the contact piece is mounted on or in the base of the crucible and is constructed as a crucible mounting.
2. The apparatus according to claim 1, characterized in that the capillary is guided through the base of the crucible.
3. The apparatus according to claim 1 or 2, characterized in that the inner diameter of the capillary is widened at the nozzle.
4. The apparatus according to claim 1 or 2, characterized in that the nozzle is constructed in a slit shape.
5. The apparatus according to any one of claims 1 to 4, characterized in that the difference between the inner and outer diameter of the capillary on the outer end of the nozzle is not greater than 1 mm.
6. The apparatus according to claim 5, characterized in that the difference is not greater than 0.5 mm.
7. The apparatus according to any one of claims 1 to 6, characterized in that the product of thermal conductivity and wall thickness of the capillary at the outer end of the nozzle is smaller than 5.5 x 10 3 W/K at 1400°C.
8. The apparatus according to claim 3 or 4, characterized in that the nozzle is arranged laterally on the capillary.
9. The apparatus according to any one of claims 1 to 8, characterized in that the capillary is formed from a gas-tight material.
10. The apparatus according to claim 9, wherein the gas-tight material is selected from the group consisting of aluminium oxide, quartz and zirconium oxide.
11 11. A measuring apparatus with a gas pipe and with a device for measuring the surface tension of fluids with a capillary for a gas supply, the capillary having a contact piece and a nozzle in which the capillary is at least partially arranged in a crucible to receive the fluid and in which the contact piece is arranged outside the interior of the crucible, in which the capillary is guided through a wall of the crucible and is mounted on the wall of the crucible, in which the contact piece is mounted on or in the base of the crucible and is constructed as a crucible mounting and connected in a gas-tight manner with a gas connection piece of the gas pipe and also with a pressure sensor and with a through-flow meter.
12. A measuring apparatus with a gas pipe, and with a device for measuring the surface tension of fluids with a capillary for a gas supply, the capillary having a contact piece and a nozzle, in which the capillary is at least partially arranged in a crucible to receive the fluid and in which the contact piece is arranged outside the interior of the crucible, in which the capillary is guided through a wall of the crucible and is mounted on the wall of the crucible, in which the contact piece is mounted on or in the base of the crucible and is constructed as a crucible mounting and connected in a gas-tight manner with a gas connection piece of the gas pipe and also with a pressure sensor or with a through-flow meter.
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE4423720A DE4423720C1 (en) | 1994-07-08 | 1994-07-08 | Surface tension measurement esp. in molten metal |
| DEP4423720.0 | 1994-07-08 | ||
| EP95106682A EP0694779B1 (en) | 1994-07-08 | 1995-05-04 | Device for measuring surface tension |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2153286A1 CA2153286A1 (en) | 1996-01-09 |
| CA2153286C true CA2153286C (en) | 2005-11-22 |
Family
ID=25938062
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002153286A Expired - Fee Related CA2153286C (en) | 1994-07-08 | 1995-07-05 | Apparatus for measuring surface tension |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP0694779B1 (en) |
| JP (1) | JP3599432B2 (en) |
| CA (1) | CA2153286C (en) |
| DE (1) | DE4423720C1 (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE29609646U1 (en) * | 1996-05-31 | 1996-08-14 | Technische Universität Dresden, 01069 Dresden | Device for the dynamic measurement of the surface tension of a liquid |
| DE10110213B4 (en) * | 2001-03-04 | 2006-12-21 | Sita Messtechnik Gmbh | Capillary and measuring device for determining the surface or interfacial tension of a liquid |
| DE10304603B4 (en) * | 2002-02-13 | 2011-01-13 | Sita Messtechnik Gmbh | measuring capillary |
| DE10346780A1 (en) * | 2003-10-08 | 2005-05-25 | Daimlerchrysler Ag | Iron melt quality measurement comprises use of surface wave excitation and detects wave attenuation to assess impurity concentration and graphite precipitation |
| DE10346781A1 (en) * | 2003-10-08 | 2005-05-25 | Daimlerchrysler Ag | Iron melt quality measurement comprises use of surface tension measurement to assess impurity concentration and graphite precipitation |
| CN101082558B (en) * | 2007-07-16 | 2010-05-26 | 哈尔滨理工大学 | Anti-disturbance device for rapid detection of fluctuating melt surface tension |
| DE102007056669A1 (en) * | 2007-11-24 | 2009-05-28 | Krüss GmbH, Wissenschaftliche Laborgeräte | Method and apparatus for the rapid formation of fluid interfaces and use of this apparatus for the determination of liquid-liquid and liquid-gas interface properties |
| RU2691764C1 (en) * | 2018-05-07 | 2019-06-18 | федеральное государственное бюджетное образовательное учреждение высшего образования "Марийский государственный университет" | Device for formation of spherical surface of liquid for determination of surface tension coefficient |
Family Cites Families (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR1341670A (en) * | 1962-09-20 | 1963-11-02 | Thomson Houston Comp Francaise | Improvements to fusion devices |
| US3780568A (en) * | 1971-07-27 | 1973-12-25 | Ibm | Quantitative test method for measuring solder-flux surface tension interaction |
| DE2635373C2 (en) * | 1975-08-08 | 1982-04-15 | PCUK-Produits Chimiques Ugine Kuhlmann, 92400 Courbevoie, Hauts-de-Seine | Method and device for the continuous growth of single crystals of a specific shape |
| FR2393610A1 (en) * | 1977-06-09 | 1979-01-05 | Automatis Regul Appar Mes Et | REUSABLE EXPERIMENTATION CRUCIBLE |
| DE2915956A1 (en) * | 1979-04-20 | 1980-11-06 | Licentia Gmbh | Electrically conductive fluid surface tension measurement - uses electrical contacts to record flow through capillary tube |
| US4527421A (en) * | 1984-01-13 | 1985-07-09 | The Dow Chemical Company | Dynamic surface tensiometry and method |
| DE4228942C1 (en) * | 1992-08-31 | 1994-01-20 | Martin Reck | Fluid surface tension measuring system - uses detection and evaluation of gas bubbles at liquid surface caused by introduced gas |
-
1994
- 1994-07-08 DE DE4423720A patent/DE4423720C1/en not_active Expired - Fee Related
-
1995
- 1995-05-04 EP EP95106682A patent/EP0694779B1/en not_active Expired - Lifetime
- 1995-07-05 CA CA002153286A patent/CA2153286C/en not_active Expired - Fee Related
- 1995-07-07 JP JP19400995A patent/JP3599432B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| EP0694779A1 (en) | 1996-01-31 |
| JP3599432B2 (en) | 2004-12-08 |
| JPH0843290A (en) | 1996-02-16 |
| CA2153286A1 (en) | 1996-01-09 |
| EP0694779B1 (en) | 1997-07-30 |
| DE4423720C1 (en) | 1996-02-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| AU647021B2 (en) | Continuous-use molten metal inclusion sensor | |
| US7635220B2 (en) | Device for measuring cooling/heating curves of molten masses | |
| CN102460098B (en) | Insertion probe | |
| CA2153286C (en) | Apparatus for measuring surface tension | |
| KR0157222B1 (en) | Single-ues disposable molten metal inclusion sensor | |
| BRPI1102946A2 (en) | measuring probes for measuring and taking samples with a molten metal | |
| JP2009156867A (en) | Container for molten metal, use of the container and method for determining the interface layer | |
| KR100205976B1 (en) | Sensor unit for temperature measurement | |
| US5661234A (en) | Apparatus for measuring surface tension | |
| US6603296B2 (en) | Apparatus for the detection and measurement of particulars in molten metal | |
| JP2606734B2 (en) | Apparatus and method for measuring gas content of liquid metal and probe used therein | |
| JP2018506714A (en) | Reverse filled carbon and temperature drop-in sensor | |
| US6071466A (en) | Submergible probe for viewing and analyzing properties of a molten metal bath | |
| CZ377292A3 (en) | Stopper for a metallurgical casting vessel | |
| CN107209088B (en) | Reversely charging carbon and temperature fall into formula sensor | |
| US3390568A (en) | Apparatus for determining the carbon content of metals | |
| JPH0259629A (en) | Continuous temperature measuring instrument for molten metal | |
| JPH0238932A (en) | Continuous temperature measuring method for molten metal | |
| JPH0792158A (en) | Molten metal sampling device | |
| JPH04325620A (en) | Oxygen blowing nozzle for RH vacuum degassing equipment | |
| KR19990024804U (en) | Slag thickness measuring device in ladle |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EEER | Examination request | ||
| MKLA | Lapsed |
Effective date: 20150706 |