CN204855278U - Metal material young modulus measuring device based on mode natural frequency - Google Patents

Abstract

The utility model provides a metal material young modulus measuring device based on mode natural frequency, the device involving vibrations noise test system, modal analysis system, power hammer, acceleration sensor, electronic scale, ruler, young modulus computational system, rack, rubber rope, length are L's test piece, and the device's connected mode is: the rubber rope hangs on the rack for the test piece, and the position that the test piece hung is 0.224L and 0.776L respectively apart from test piece left end face, fixed acceleration sensor on the test piece to link to each other acceleration sensor with vibration noise test system with the wire, will do all can the hammer with the wire and link to each other with vibration noise test system, with the wire will vibrate the noise test system, the modal analysis system links to each other with young modulus computational system. The utility model discloses a test result combines the theoretical equation to derive metal material's young modulus, makes young modulus property value deterministic process accurate, high -efficient.

Description

Based on the metal material young modulus measuring device of Modal frequency

Technical field

The utility model relates to a kind of metal material young modulus measuring device based on Modal frequency, concrete finger, by measuring first natural frequency under test specimen free state and binding isotherm formulae discovery, is tested and derives the detection method of metal material Young modulus.

Background technology

Young modulus is an important parameter of reflection characteristic of material mechanics, when carrying out finite element simulation research to mechanical structured member, provide the accuracy of the Young modulus of material by the accuracy of direct impact analysis result, therefore by experiment method to obtain the Young modulus of material very important.In recent years, in field of engineering technology, the Young modulus of many employings optical lever method measuring metallic materials, need to prepare thinner tinsel when carrying out this measurement test, when measuring wire length L, because tinsel upper and lower side is equipped with mounting bracket, tinsel is in vertical elongated condition simultaneously, series of problems can be brought: one is the obstruction due to mounting bracket when measuring, steel tape is difficult to press close to tinsel, steel tape just can must be measured with tinsel Parallel offset certain distance, due to the parallax of human eye reading, can reduce reading accuracy; Secondly, because tinsel is in vertical elongated condition, gauger removes reading after steel tape vertically will being elongated again, is difficult to ensure that sight line is alignd with scale, thus produces parallax, reduces reading accuracy; 3rd, due to have employed optical lever repeatedly imaging method amplify micro-displacement, so the small sample perturbations to original displacement, also can zoom into sizable interference simultaneously, thus affect the degree of accuracy of reading numerical values.Measurement for metal material Young modulus also has multiple method, as Fiber Optical Sensor Based, CCD method, interferometric method, pulling method and diffraction approach etc., but the most experimental implementation of these methods is loaded down with trivial details, theoretical formula is complicated, cause measuring low, the on-the-spot bad adaptability of efficiency, therefore need the new Young modulus of device to metal material of research to measure.

Summary of the invention

Technical problem to be solved in the utility model is, provide a kind of can simplified measurement process, reduce and measure cost, improve the metal material young modulus measuring device of measurement result accuracy.

The technical solution of the utility model is: a kind of metal material young modulus measuring device based on Modal frequency, this device involving vibrations noise measuring system, modal analysis system, power is hammered into shape, acceleration transducer, electronic scales, ruler, Young modulus computing system, stand, elastic string, length is the test specimen of L, the connected mode of this device is: test specimen elastic string is suspended on stand, the position that test specimen hangs is respectively 0.224L and 0.776L apart from test specimen left side, acceleration transducer fixed by test specimen, and be connected with vibration and noise test system with wire degree of will speed up sensor, with wire, power hammer is connected with vibration and noise test system, with wire by vibration and noise test system, modal analysis system is connected with Young modulus computing system, test process is: firmly hammer knocks test specimen, the acceleration responsive of each measuring point of acceleration transducer pickup test specimen, this response signal imports vibration and noise test system, modal analysis system and Young modulus computing system into, obtains the Young modulus of first natural frequency under this test specimen free state and material.

The above-mentioned metal material young modulus measuring device based on Modal frequency, its length is the test specimen of L is uniform cross section round bar shape.

The above-mentioned metal material young modulus measuring device based on Modal frequency, test specimen natural frequency test process is: a point of excitation is got in the test specimen one end being L in length, in all the other positions of test specimen by equidistant placement acceleration transducer, firmly hammer is made to knock test specimen, the acceleration responsive of each measuring point of acceleration transducer pickup test specimen, this response signal imports vibration and noise test system and modal analysis system into, solve the modal parameter of test specimen with least square fitting, the first natural frequency f under test specimen free state can be obtained ₁.

The above-mentioned metal material young modulus measuring device based on Modal frequency, the process of asking for of test specimen Young modulus is: first natural frequency f under piece lengths L, test specimen diameter d, test specimen quality m and test specimen free state ₁young modulus computing system is imported into, according to formula etc. parameter obtain the Young modulus of material for test.

Theoretical foundation based on Modal frequency measuring metallic materials Young modulus:

The transverse vibration of cylinder beam in xoy plane, as shown in Fig. 2 (a), discusses the situation that transversely deforming y (x, t) is only caused by moment of flexure now.Consider the free body diagram of the infinitesimal dx shown in Fig. 2 (b), by Newton second law, horizontal dynamic force equation is

$\mathrm{\ρ}S\frac{{\∂}^{2}y}{\∂t^2}dx=-\left(Q+\frac{Qy}{\∂x}dx\right)+Q$ Or $m\frac{{\∂}^{2}y}{\∂t^2}=-\frac{\∂Q}{\∂x}---\left(1\right)$

In formula, the density of ρ-cylinder beam, S-cylinder beam section amasss, Q-shearing.

Infinitesimal dx right flank moment of flexure that place has is added and draws

$\frac{\∂M}{\∂x}\mathrm{dx}-\mathrm{Qdx}\≈0$ Or $\frac{\∂M}{\∂x}=Q---\left(2\right)$

From mechanics of materials knowledge, the curvature of cylinder beam and the pass of moment of flexure are

$EJ\frac{{\∂}^{2}y}{\∂x^2}=M---\left(3\right)$

In formula, the elastic modulus of E-cylinder beam material, J=∫ ∫ _sy ²ds is called the inertia square (depending on the shape in cross section) in a certain cross section, the inertia square J=S (d/4) of cylinder beam ², wherein d is the diameter of cylinder beam, M-moment of flexure.

Formula (2) combined with formula (3), the equation of motion of cylinder beam transverse vibration can be written as

$\mathrm{\ρ}S\frac{{\∂}^{2}y}{\∂t^2}=-\frac{{\∂}^2}{\∂x^2}\left(EJ\frac{{\∂}^{2}y}{\∂x^2}\right)---\left(4\right)$

To the cylinder beam of a length L > > diameter d, lifted with two suspension wires at middle part, as shown in Figure 1, two ends are made to be in free state, do not considering in external force situation, the displacement in x place vertically (y direction) meets following relation:

$\frac{{\∂}^{4}y}{\∂x^4}+\frac{\mathrm{\ρ}S}{EJ}\·\frac{{\∂}^{2}y}{\∂t^2}=0---\left(5\right)$

With partition method solving equation (5), make y (x, t)=X (x) T (t), substitute into formula (5), can obtain

$\{\begin{array}{c}\frac{d^{4}X}{{\mathrm{dx}}^4}-K^{4}X=0\\ \frac{d^{2}T}{{\mathrm{dt}}^2}+\frac{K^{4}EJ}{\mathrm{\ρ}s}T=0\end{array}---\left(6\right)$

If each point all does simple harmonic motion on cylinder beam, then the general solution of this two equation is respectively

$\{\begin{array}{c}X\left(x\right)=a_{1}chKx+a_{2}shKx+a_3\cos Kx+a_4\sin Kx\\ T\left(t\right)=b\cos \left(\mathrm{\ω}t+\mathrm{\φ}\right)\end{array}---\left(7\right)$

So the general solution of Crosswise Vibration Equation (5) is

y(x，t)＝(a ₁chKx+a ₂shKx+a ₃cosKx+a ₄sinKx)·bcos(ωt+φ)(8)

In formula

$\mathrm{\ω}={\left(\frac{K^{4}EJ}{\mathrm{\ρ}s}\right)}^{\frac{1}{2}}---\left(9\right)$

Be called inherent circular frequency formula, be applicable to the test specimen of Tension Members with Arbitrary Shape Section under various boundary.As long as make constant K with specific boundary condition, bring the inertia square J of particular cross section into, just can obtain the computing formula under actual conditions.If suspension wire is suspended near the node (being in the cylinder beam of resonance state, the position of displacement identically vanishing) of test specimen, then the two ends of cylinder beam are all in free state.Now its boundary condition is that free end horizontal force F and moment M are zero.Namely

$F=-EJ\frac{d^{3}y}{{\mathrm{dx}}^3}=0$

$M=EJ\frac{d^{2}y}{{\mathrm{dx}}^2}=0$

Therefore have

$\frac{d^{3}X}{{\mathrm{dx}}^3}{|}_{x=0}=0\frac{d^{3}X}{{\mathrm{dx}}^3}{|}_{x=L}=0\frac{d^{2}X}{{\mathrm{dx}}^2}{|}_{x=0}=0\frac{d^{2}X}{{\mathrm{dx}}^2}{|}_{x=L}=0$

General solution is brought into and obtains with upper boundary conditions

cosKL·chKL＝1(10)

Employing numerical solution can obtain eigen value K and cylinder beam length L should meet

$K_{n}L=0,4.730,7.853,10.996,...,\left(n+\frac{1}{2}\right)\mathrm{\π}$

Work as K ₁l=4.730, time corresponding test specimen frequency be exactly the first rank non-zero inherent circular frequency under free state.Test specimen there are two nodes with during the first rank non-zero natural frequency vibration, their position distance left end 0.224L and 0.776L respectively.

By first eigenvalue K ₁the K that L=4.73 is corresponding ₁=4.73/L substitutes into formula (9), and the first rank non-zero inherent circular frequency when can obtain free vibration is

${\mathrm{\ω}}_1={\[\frac{{4.730}^{4}EJ}{L^4\mathrm{\ρ}s}\]}^{\frac{1}{2}}---\left(11\right)$

Solve Young modulus $E=1.9978\×{10}^{-3}\·\frac{{\mathrm{\ρsL}}^4}{J}\·{\mathrm{\ω}}_1^2=7.8870\×{10}^{-2}\·\frac{L^{3}m}{J}\·f_1^2---\left(12\right)$

In formula: it is the first rank non-zero natural frequency.

For cylinder beam $J=\underset{s}{\∫}{y}^{2}dS=S{\left(\frac{d}{4}\right)}^2=\frac{{\mathrm{\πd}}^4}{64}$

Substitution above formula obtains $E=1.6067\frac{L^{3}m}{d^4}{f}_1^2---\left(13\right)$

In formula: m is the quality of cylinder beam.Formula (13) is the computing formula of this experiment Young modulus.In International System of Units, the unit of Young modulus E is Nm ^-2.

Helpfulness of the present utility model is by obtaining natural frequency value accurately to the test of test specimen hammering method, the Young modulus actual numerical value of test specimen metal material can be obtained in conjunction with Young modulus theoretical formula, this when do not have Material Testing Machine or needs to obtain Young modulus is to solve site problems accurately be particularly useful, the utility model can simplified measurement process, reduce and measure cost, improve the accuracy of measurement result.

Accompanying drawing explanation

Fig. 1 is the metal material young modulus measuring device composition diagram based on natural frequency representing an embodiment of the present utility model.

Fig. 2 is the cylinder beam transverse vibration schematic diagram representing the utility model theoretical foundation.

Fig. 3 is the metal material Young modulus Measurement and analysis process flow diagram representing the above-mentioned embodiment of the utility model.

Drawing reference numeral explanation

1, vibration and noise test system, 2, modal analysis system, 3, power hammer, 4, acceleration transducer, 5, electronic scales, 6, ruler, 7, Young modulus computing system, 8, stand, 9, bungee, 10, test specimen

Embodiment

Below, 1 ~ 3 the metal material young modulus measuring device based on natural frequency of the present utility model is described in detail below by reference to the accompanying drawings.

As shown in Figure 1 based on metal material young modulus measuring device involving vibrations noise measuring system 1, modal analysis system 2, power hammer 3, acceleration transducer 4, electronic scales 5, ruler 6, Young modulus computing system 7, stand 8, bungee 9, the test specimen 10 of Modal frequency, metal material Young modulus measuring method is as follows:

A) length L and the diameter d of test specimen 10 is measured with ruler 6;

B) the quality m of test specimen 10 is measured with electronic scales 5;

C) be suspended on stand 8 by test specimen 10 elastic string 9, the position that test specimen hangs is apart from test specimen left side 0.224L and 0.776L;

D) on test specimen 10, fix acceleration transducer 4, and be connected with vibration and noise test system 1 with wire degree of will speed up sensor 4;

E) with wire, power hammer 3 is connected with vibration and noise test system 1;

F) vibration and noise test system 1, modal analysis system 2 are connected with Young modulus computing system 7;

G) point of excitation is got in one end of test specimen 10, in all the other positions of test specimen by equidistant placement acceleration transducer 4, firmly hammer 3 is made to knock test specimen 10, acceleration transducer 4 picks up the acceleration responsive of each measuring point of test specimen 10, power hammers 3 pickup force signals into shape, solves the first natural frequency value f of test specimen 10 with least square fitting ₁.

H) by test specimen 10 length L, diameter d, quality m and first natural frequency f ₁import Young modulus computing system 7 into, according to formula namely the Young modulus value of test specimen is obtained.

Claims (2)

1. the metal material young modulus measuring device based on Modal frequency, this device involving vibrations noise measuring system, modal analysis system, power is hammered into shape, acceleration transducer, electronic scales, ruler, Young modulus computing system, stand, elastic string, length is the test specimen of L, the connected mode of this device is: test specimen elastic string is suspended on stand, the position that test specimen hangs is respectively 0.224L and 0.776L apart from test specimen left side, acceleration transducer fixed by test specimen, and be connected with vibration and noise test system with wire degree of will speed up sensor, with wire, power hammer is connected with vibration and noise test system, with wire by vibration and noise test system, modal analysis system is connected with Young modulus computing system, test process is: firmly hammer knocks test specimen, the acceleration responsive of each measuring point of acceleration transducer pickup test specimen, this response signal imports vibration and noise test system, modal analysis system and Young modulus computing system into, obtains the Young modulus of first natural frequency under this test specimen free state and material.

2. the metal material young modulus measuring device based on Modal frequency according to claim 1, is characterized in that length be the test specimen of L is uniform cross section round bar shape.