PL112319B2 - Method for measurement of elasticity constants - Google Patents
Method for measurement of elasticity constants Download PDFInfo
- Publication number
- PL112319B2 PL112319B2 PL20126277A PL20126277A PL112319B2 PL 112319 B2 PL112319 B2 PL 112319B2 PL 20126277 A PL20126277 A PL 20126277A PL 20126277 A PL20126277 A PL 20126277A PL 112319 B2 PL112319 B2 PL 112319B2
- Authority
- PL
- Poland
- Prior art keywords
- resonance
- constant
- vibrations
- sample
- frequencies
- Prior art date
Links
- 238000000034 method Methods 0.000 title claims description 9
- 238000005259 measurement Methods 0.000 title 1
- 239000000463 material Substances 0.000 claims description 3
- 230000004936 stimulating effect Effects 0.000 claims description 2
- 238000005452 bending Methods 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 210000000988 bone and bone Anatomy 0.000 description 1
- 238000012885 constant function Methods 0.000 description 1
- 238000009774 resonance method Methods 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
Landscapes
- Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)
Description
Przedmiotem wynalazku jest sposób pomiaru stalych sprezystosci metoda rezonansu akustycznego.Znany jest z opisu patentowego PRL nr 62032 sposób pomiaru stalych sprezystosci wedlug którego badana próbka podparta w czterech punktach lezacych na liniach wezlowych powierzchni drgajacej pobudzanajest do drgan wlasnych pierwszego i drugiego rzedu a wiel¬ kosc stalych sprezystosci okresla sie oznaczeniem sto¬ sunku czestotliwosci drugiego rezonansu drgan wlasnych do czestotliwosci pierwszego rezonansu tych drgan.Istota sposobu wedlug wynalazku polega na tym, ze badana próbke w postaci plyty kolowej podpartej w trzech wezlach drgan pobudza sie bezstykowa metoda pojemnosciowa do drgan wlasnych drugiego i trzeciego rzedu i drgania te odbiera sie za pomoca bezstykowego przetwornika odbiorczego. Wielkosc stalych sprezystosci okresla sie bezposredniooznaczeniem stosunku czestotli¬ wosci drugiego rezonansu drgan wlasnych do czestotli¬ wosci trzeciego rezonansu tych drgan.Sposób wedlug wynalazku zapewnia stabilne poloze¬ nie próbki nawet w przypadku jej deformacji wywolanej duzymi zmianami temperatury.Sposób pomiaru stalych sprezystosci zostanie blizej objasniony w oparciu o rysunek przedstawiajacy na fig. 1 obraz linii wezlowych drugiego rezonansu na badanej próbce kolistej, na fig. 2 — obraz linii wezlowych trze¬ ciego rezonansu tej samej próbki, a fig. 3 — rozmieszcze¬ nie punktów podparcia plytki.Badana próbka kolista podpartajest przez stalowe igly w trzech punktach W lezacych na liniach wezlowych powierzchni drgajacej próbki. W próbce tej wzbudza sie rezonans fal gietnych drugiego rzedu fi tj. taki wktórym linie wezlowe maja postac okregu po czym w próbce wzbudzany jest rezonans fal gietnych trzeciego rzedu f 3tj. taki w którym linie wezlowe maja postac trzech przecina¬ jacych sie srednic.Punkty zamocowania próbki W znajduja sie na prze¬ cieciu linii wezlowych rezonansów f2i d. Nastepnie mierzy sie czestotliwosc drgan przy którym nastepuje rezonans U i f3 i stosunek czestotliwosci drgan drugiego rezonansudo czestotliwosci drgan trzeciego rezonansujest funkcja sta¬ lej Poissona. Znajac wymiary geometryczne badanej próbki oraz gestosc badanego materialu po zmierzeniu stalej Poissona wyznacza sie modul sprezystosci E.Zastrzezenie patentowe Sposób pomiaru stalych sprezystosci materialów pole¬ gajacy napobudzaniu próbki do drgan wlasnych i wyzna¬ czaniu stalych sprezystosci na podstawie czestotliwosci rezonansowych, znamienny tym, ze badana próbke zamo¬ cowana w trzech punktach (W) znajdujacych sie na liniach wezlowych rezonansów (f2 i f3 pobudza sie do gietnych drgan rezonansowych drugiego rzedu (f2 i trze¬ ciego rzedu (f 3) i mierzy sie czestotliwosci tych drgan przy czym stale sprezystosci okreslasie oznaczeniem stosunku tych czestotliwosci.\\2 M9 Fig4 Bg.2 Fig.5 Prac. Poligraf. UP PRL. Naklad 120 egz.Cena 45 zl PLThe subject of the invention is a method of measuring constant resonance using the acoustic resonance method. It is known from the patent description of the Polish People's Republic No. 62032 a method of measuring constant resistances, according to which the tested sample supported at four points lying on the knot lines of the vibrating surface is stimulated to the own vibrations of the first and second order and the magnitude of the constant bones the resonance is determined by the ratio of the frequency of the second resonance of natural vibrations to the frequency of the first resonance of these vibrations. The essence of the method according to the invention consists in the fact that the tested sample in the form of a circular plate supported in three vibration nodes stimulates the contactless capacitive method to vibration of the second natural row and these vibrations are perceived by a contactless pickup transducer. The magnitude of the constant resonance is directly determined by the ratio of the frequency of the second resonance to the frequency of the third resonance of these vibrations. The method according to the invention ensures a stable position of the sample even in the case of its deformation caused by large changes in temperature. The method of measuring constant resonance will be closer to the frequency of the third resonance of these vibrations. Fig. 1 shows the image of the second resonance node lines on the test circular sample, in Fig. 2 the image of the third resonance node lines of the same sample, and Fig. 3 the arrangement of the plate support points. The test circular sample is supported by through steel needles at three points W lying on the knot lines of the vibrating surface of the sample. In this sample, the resonance of bending waves of the second order fi is induced, i.e. one in which the knot lines have the form of a circle, and then in the sample the resonance of bending waves of the third order f3tj is induced. one in which the node lines have the form of three intersecting diameters. The fixing points of the sample W are located at the intersection of the node lines of the resonances f2 and d. Then the vibration frequency is measured with the resonance U and f3 and the vibration frequency ratio of the second resonance to the vibration frequency the third resonance is the Poisson constant function. Knowing the geometrical dimensions of the test sample and the density of the tested material, after measuring the Poisson constant, the modulus of elasticity E is determined. Patent disclaimer The method of measuring the constant elasticity of materials consisting in stimulating the sample to its own vibration and determining the constant elasticity on the basis of resonance frequencies, characterized by the fact that the tested the sample is attached to three points (W) located on the nodal lines of the resonances (f2 and f3 stimulate high resonance vibrations of the second order (f2 and third order (f 3) and the frequency of these vibrations is measured, with the elasticity constant being determined by designation of the ratio of these frequencies. \\ 2 M9 Fig4 Bg.2 Fig. 5 Printed work of the Polish People's Republic of Poland. Circulation 120 copies Price PLN 45 PL
Claims (2)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PL20126277A PL112319B2 (en) | 1977-10-03 | 1977-10-03 | Method for measurement of elasticity constants |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PL20126277A PL112319B2 (en) | 1977-10-03 | 1977-10-03 | Method for measurement of elasticity constants |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| PL201262A1 PL201262A1 (en) | 1978-08-14 |
| PL112319B2 true PL112319B2 (en) | 1980-10-31 |
Family
ID=19984883
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PL20126277A PL112319B2 (en) | 1977-10-03 | 1977-10-03 | Method for measurement of elasticity constants |
Country Status (1)
| Country | Link |
|---|---|
| PL (1) | PL112319B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| PL221046B1 (en) | 2009-06-03 | 2016-02-29 | Janusz Moszczański | Method and device for obtaining composites from thermoplastics waste |
| EP3842482A1 (en) | 2019-12-23 | 2021-06-30 | Maciej Adam Dechnik | Ecological composite made of recycled thermoplastic materials and method used in its production |
-
1977
- 1977-10-03 PL PL20126277A patent/PL112319B2/en unknown
Also Published As
| Publication number | Publication date |
|---|---|
| PL201262A1 (en) | 1978-08-14 |
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