SU864057A1 - Method of determining electroconductive material thermal stability - Google Patents
Method of determining electroconductive material thermal stability Download PDFInfo
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- SU864057A1 SU864057A1 SU792862216A SU2862216A SU864057A1 SU 864057 A1 SU864057 A1 SU 864057A1 SU 792862216 A SU792862216 A SU 792862216A SU 2862216 A SU2862216 A SU 2862216A SU 864057 A1 SU864057 A1 SU 864057A1
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Description
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Изобретение относитс к исследовани м прочностных свойств матери.алов , а именно к способам определени термостойкости электропровод щих материалов .The invention relates to the study of the strength properties of material materials, and specifically to methods for determining the heat resistance of electrically conductive materials.
Известен способ определени термостойкости электропровод щих материалов , заключающийс в том, что создают градиент температур по толщине образца материала при нагреве его пропусканием импульса электрического тока, измер ют температуру образца и врем от начала пропускани тока до момента разрушени образца Щ.A known method for determining the heat resistance of electrically conductive materials, which consists in creating a temperature gradient across the thickness of a sample of a material when heated by passing an electric current pulse, measures the temperature of the sample and the time from the beginning of the current passing until the sample breaks.
Недостатком данного способа вл етс низка точность определени термостойкости .The disadvantage of this method is the low accuracy of the determination of heat resistance.
Цель изобретени - повышение точности определени .The purpose of the invention is to improve the accuracy of determination.
Указанна цель достигаетс тем, что измер ют врем ТплОг начгша пропускани тока до момента начала плавлени материала образца и врем 1Гр от момента начала плавлени до момента разрушени образца, а термостойкость определ ют по отношению Tp/t jy. Кроме того, измер ют также электропроводность и уровень акустической эмиссии образца, о ыоме те начала плавлени материала образца суд т по скачку электропроводности, а о моменте разрушени - по изменению . уровн акустической эмиссии от образца .This goal is achieved by measuring the time TplOg of the start of current flow until the beginning of the melting of the sample material and the time 1Gy from the time of the start of melting to the moment of the sample destruction, and the heat resistance is determined by the ratio Tp / t jy. In addition, the electrical conductivity and the level of acoustic emission of the sample are also measured, the occurrence of the initial melting of the material of the sample is judged by the jump in electrical conductivity, and the moment of destruction is determined by the change. the level of acoustic emission from the sample.
J Способ осуществл ют следующим образом.J The method is carried out as follows.
Исследуемый образец, изготовленный в виде двух пластин / зажимают между двум массивными охлаждаемымиA test specimen manufactured in the form of two plates / clamped between two massive cooled
10 электродами. Когда через образец пропускают импульс электрического тока, на контактном сопротивлении в месте соприкосновени выдел етс тепло, что приводит к скачкообразному повышению температуры, при этом образец испытывает тепловой удар. После окончани импульса тока происходит охлаждение нагретой части образца. В процессе испытани измер ют электропроводность материала образца. Момент достижени материалом образца температуры плавлени определ етс по скачку электропроводности. Локальное плавление материала образца может быть определено, например, по нгшичию максимума на осциллограмме импульса тока, пропускаемого через образец. Момент разрушени образца определ ют по изменению уровн акустической эмиссии от образца, которую10 electrodes. When a pulse of electric current is passed through the sample, heat is generated at the contact resistance at the point of contact, which causes an abrupt rise in temperature, and the sample experiences thermal shock. After the end of the current pulse, the heated portion of the sample is cooled. During the test, the electrical conductivity of the sample material is measured. The moment when the sample material reaches the melting point is determined by the jump in electrical conductivity. The local melting of the sample material can be determined, for example, by the maximum of the oscillogram of the current pulse transmitted through the sample. The moment of destruction of the sample is determined by the change in the level of acoustic emission from the sample, which
также измер ют в процессе испытани . Термостойкость определ етс отношением времени от начала плавлени до момента разрушени образца ко времени от начала пропускани тока до начаг;а плавлени .also measured during the test. The heat resistance is determined by the ratio of the time from the beginning of melting to the moment of the destruction of the sample to the time from the beginning of the passage of current to the beginning and melting.
Предлагаемый способ определени термостойкости электропровод щих материалов повышает точность определени , учитыва врем разогрева материала , которое определ ет скорость термического разрушени .The proposed method for determining the heat resistance of electrically conductive materials improves the determination accuracy, taking into account the heating time of the material, which determines the rate of thermal destruction.
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Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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SU792862216A SU864057A1 (en) | 1979-12-27 | 1979-12-27 | Method of determining electroconductive material thermal stability |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
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SU792862216A SU864057A1 (en) | 1979-12-27 | 1979-12-27 | Method of determining electroconductive material thermal stability |
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SU864057A1 true SU864057A1 (en) | 1981-09-15 |
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SU792862216A SU864057A1 (en) | 1979-12-27 | 1979-12-27 | Method of determining electroconductive material thermal stability |
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1979
- 1979-12-27 SU SU792862216A patent/SU864057A1/en active
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