- About this Journal ·
- Abstracting and Indexing ·
- Aims and Scope ·
- Annual Issues ·
- Article Processing Charges ·
- Author Guidelines ·
- Bibliographic Information ·
- Citations to this Journal ·
- Contact Information ·
- Editorial Board ·
- Editorial Workflow ·
- Free eTOC Alerts ·
- Publication Ethics ·
- Recently Accepted Articles ·
- Reviewers Acknowledgment ·
- Submit a Manuscript ·
- Subscription Information ·
- Table of Contents
Advances in Materials Science and Engineering
Volume 2013 (2013), Article ID 329530, 6 pages
Flexural Vibration Test of a Beam Elastically Restrained at One End: A New Approach for Young’s Modulus Determination
Faculty of Aerospace Engineering, Technion—Israel Institute of Technology, 32000 Haifa, Israel
Received 1 May 2013; Accepted 11 July 2013
Academic Editor: Xing Chen
Copyright © 2013 Rafael M. Digilov and Haim Abramovich. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
A new vibration beam technique for the fast determination of the dynamic Young modulus is developed. The method is based on measuring the resonant frequency of flexural vibrations of a partially restrained rectangular beam. The strip-shaped specimen fixed at one end to a force sensor and free at the other forms the Euler Bernoulli cantilever beam with linear and torsion spring on the fixed end. The beam is subjected to free bending vibrations by simply releasing it from a flexural position and its dynamic response detected by the force sensor is processed by FFT analysis. Identified natural frequencies are initially used in the frequency equation to find the corresponding modal numbers and then to calculate the Young modulus. The validity of the procedure was tested on a number of industrial materials by comparing the measured modulus with known values from the literature and good agreement was found.
The Young modulus is a fundamental material property and its determination is common in science and engineering [1, 2]. It is a key parameter in mechanical engineering design to predict the behavior of the material under deformation forces or more to get an idea of the quality of the material. Young’s moduli are determined from static and dynamic tests. In static measurements [3, 4] such as the classical tensile or compressive test, a uniaxial stress is exerted on the material, and the elastic modulus is calculated from the transverse and axial deformations as the slope of the stress-strain curve at the origin. Dynamic methods [5–12] are more precise and versatile since they use very small strains, far below the elastic limit and therefore are virtually nondestructive allowing repeated testing of the same sample. These include the ultrasonic pulse-echo [6, 7] or bar resonance methods [4, 8–14]. In the sonic pulse technique, the dynamic Young modulus is determined by measuring the sound velocity in the sample. In the resonance method, the linear elastic, uniform, and isotropic material of density usually in the form of a bar of known dimensions is subjected to transverse or flexural vibrations, the natural frequency of th mode of which related to Young’s modulus by the relation [15, 16] can be accurately measured. In (1) is the modal eigenvalue that depends on boundary conditions, is the vibrating length of the bar, is its cross-sectional area, and is the second moment of the cross-section, equal to for a rod of radius and for a rectangular beam with width and depth . Knowing the modal numbers, by simply measuring the resonance frequencies, geometry, and density of the specimen, the Young modulus can be determined from (1) as The test sample is usually arranged in a manner to simulate free-free or clamped-free end conditions [10–12], when , associated with the flexural mode is a constant.
In the present paper, we develop a new approach, in which a rectangular strip-shaped sample attached to a force sensor forms the Euler Bernoulli beam with partial translational and rotational restraints at the fixed end. This feature expands the capabilities of the resonant beam method making it suitable for materials with high stiffness and low density in which case, it is difficult to ascertain the flexural resonance frequencies with high certainty.
2. Theoretical Background
Consider a rectangular bar of uniform density , cross-section dimensions of which width and depth are much less than length . The bar is fixed at one end to the force sensor with a linear and torsion springs constants (see Figure 1) and is otherwise free to move in the transverse z-direction. For small deflections, that is, , the effects of rotary inertia and shear deformation can be ignored. In this case, neglecting the deflection due to the weight, the flexural displacement of a bar, at point is governed by the Euler-Bernoulli equation  with boundary conditions at : which correspond to the force and moment balance, respectively. At the free end there are no moment and shear force acting, that is, Equations (3)–(5) define completely the linear flexural vibration problem, in which the natural frequencies of the beam depend on spring constants and . Applying the separation of variables method, the solution of (3) can be cast in the following form: where describes the normal mode and (=, : resonant frequency) is the angular frequency of the mode. Substituting (6) into (3) gives an eigenvalue problem in the form of a fourth-order ordinary differential equation where is related to the angular frequency and the modal number by the dispersion relationship With the boundary condition, (4), the solution of (7) admits the form of flexural eigenmode: where related coefficients and are defined as with and expressed through experimentally accessible quantities: and integration constants and are related by the modal restriction equation (5) as where the second equality implies the constraints on possible values of , known as the frequency equation: For given values of and , transcendental equation (13) has infinite (iterative or graphical) solutions. As and (13) becomes that is the frequency equation for the free-free beam. For (13) reduces to the frequency equation derived by Chun , which in our case is written in the form which, in turn, at becomes the frequency equation for the clamped-free beam
3. Principles of Operation
The experimental setup consists of a commercial, Fourier Force Sensor DT 272 with rotation (=17.837 N·m) and translation (=6400 N·m−1) spring constants, accuracy , and resolution (12 bit) for a scale range . The force sensor mounted on a support is connected through data acquisition system and data studio software to a personal computer (PC) as is shown in Figure 2.
The strip-shaped specimen with a roughly mass of is attached horizontally to a force sensor at one end and is free at the other end. By simply displacing the free end in the transverse direction and abruptly releasing it, the sample is subjected to free flexural vibrations, so that the condition was fulfilled. At a given sample rate, the force sensor detects the dynamic response and through the data acquisition system displays the damped oscillations of the restoring force versus time (Figure 3(a)). This vibration signal is analyzed and processed by an FFT implemented in acquisition software like MultiLogPRO  providing the direct information about natural frequencies up to , which appears as single peaks in the frequency spectrum (Figure 3(b)). At this point, using data on the geometrical dimensions of the sample, its density, and spring constants of the force sensor and , identified resonance frequencies are used in (11) to calculate dimensionless parameters and . Knowing and , modal number was found from the graphical solution of (13) using the mathematical packages MATHEMATICA . The Young modulus is then determined from
The relative error of the method arises from the uncertainties in the measurement of the quantities in (17). The relative error in the density determined by the hydrostatic method is . The uncertainty in the thickness and length measurement are, respectively, and . The dispersion in the natural frequency determination is . By applying the error propagation technique, given by we find that the relative error in Young’s modulus does not exceed . The greatest inaccuracies occurred in the measurement of the spacemen dimensions.
4. Results and Discussion
To test the accuracy and validity of the present method, the effect of the sample length on the resonance frequency and Young’s modulus was studied. A commercial brass strip of width , thickness , and density = 8400 kg·m−3 was cut into samples of various length, so that one of the conditions of the Euler-Bernoulli beam theory remained unchanged, while the second ranged from 8 to 16. Since the ration (see Table 1) we used the approximated equation (15) to find the . The validity of this approach is illustrated in Figure 4, which shows that the solutions of both (15) and (13) practically coincide.
Based on the results of measurements of the natural frequencies and modal numbers presented in Table 1, a double logarithm plot of against predicted by (1) to be linear with the gradient of −2 shows that the slope of the line that best fits these data in a least-squares sense is −2.02 for the first mode and −1.94 for the second one. Based on the same set of data we show in Figure 5 the plot of the ratio versus . Most of the uncertainty in the ordinates of this plot arises from uncertainty of rather than . In the range of , the value of is constant to within the experimental uncertainties, showing that is in agreement with (1). For , that is smaller for validity of the Euler-Bernoulli beam theory, the ratio decreases (increases) with for the first (second) mode. For , the mean value of Young’s modulus lies within the range , listed in an extensive table of ASTM testing .
Below, we compare the results of measurements of elastic moduli at ambient temperature for a wide class of industrial materials with that accepted in the literature. A set of test specimens used were cut from the commercial sheet materials into strips of the thickness from 0.5 to 3.3 mm, width from 5 to 16.5 mm, and length from 15 to 30 cm. For each specimen, the length, width, and thickness were altered and the value of the Young modulus calculated by (17) for each set varied within the experimental error. Table 2 summarizes data of the specimen dimension, material density, natural frequencies, modal numbers, and Young’s modulus calculated from the first resonant frequency. It can be seen that test results are in good agreement with the accepted those in the literature data.
In all cases, identified natural frequencies of the partially restrained cantilever beam are lower than those for the clamped-free case. However, this does not necessary mean that the elastic modulus determined from these frequencies should be smaller than in ideal clamped-free case as the modal number, being in the denominator equation (17) in fourth power, decreases as well. Interestingly, the plot of versus in Figure 5 shows a linear dependence where is the first modal number for the clamped-free flexural vibrations of the beam. Taking into account (11), after substituting (19) in (17), we obtain the working equation for the Young modulus determination through the first resonance frequency of flexural vibrations of the partially restrained cantilever beam (Figure 6)
A new technique for the fast determination of the dynamic Young modulus was developed, yielding a substantial modification of the classical cantilever beam method. The procedure uses a rectangular beam, partially restrained at one end, flexural vibrations of which are detected with the aid of the force sensor. The relative experimental uncertainty is found to be less than 3%, which is mainly due to the uncertainty in the samples dimensions. The feasibility and accuracy of a new experimental procedure has been demonstrated by measuring the Young modulus for a number of test materials with different material properties. Comparison of obtained results with those accepted in the literature data is good. The relative deviation of measured values from the cited data is less than 5%. The method has potential advantages over other dynamic methods of being very simple and fast and requiring no additional equipment to excite resonance frequencies. It is particularly suitable for composite materials having a high stiffness and low density, such as carbon fiber reinforced plastic. The accuracy can be significantly improved by more precise determination of specimen dimensions.
This work was supported by the Ministry of Absorption and Immigration of Israel through the KAMEA Science Foundation.
- J. D. Lord and R. Morrell, ““Elastic modulus measurement”. Measurement good practice guide, No. 98,” Febraury 2007, http://www.npl.co.uk/publications/guides/guides-by-title/.
- J. D. Lord, Review of Methods and Analysis Software for the Determination of Modulus from Tensile Tests, vol. 41, NPL Measurement Note MATC (MN), 2002.
- P. E. Armstrong, Measurement of Mechanical Properties, Techniques of Metals Research, vol. 5, part 2 of Edited by R. F. Bunshan, John Wiley & Sons, New York, NY, USA, 1971.
- M. Radovic, E. Lara-Curzio, and L. Riester, “Comparison of different experimental techniques for determination of elastic properties of solids,” Materials Science and Engineering A, vol. 368, no. 1-2, pp. 56–70, 2004.
- A. Wolfenden, Ed., Dynamic Elastic Modulus Measurements in Materials, American Society for Testing and Materials, 1990.
- A. S. Birks and R. E. Green, Nondestructive Testing Handbook, vol. 7 of Ultrasonic Testing, American Society for Nondestructive Testing, 1991.
- A. Migliori and J. L. Sarrao, Resonant Ultrasound Spectroscopy: Applications to Physics, Materials Measurements and Nondestructive Evaluation, John Wiley & Sons, New York, NY, USA, 1997.
- A. Wolfenden, M. R. Harmouche, G. V. Blessing, et al., “Dynamic Young's modulus measurements in metallic materials: results of an interlaboratory testing programm,” Journal of Testing and Evaluation, 1989.
- G. Roebben, B. Bollen, A. Brebels, J. van Humbeeck, and O. van der Biest, “Impulse excitation apparatus to measure resonant frequencies, elastic moduli, and internal friction at room and high temperature,” Review of Scientific Instruments, vol. 68, no. 12, pp. 4511–4515, 1997.
- W. Lins, G. Kaindl, H. Peterlik, and K. Kromp, “A novel resonant beam technique to determine the elastic moduli in dependence on orientation and temperature up to 2000°C,” Review of Scientific Instruments, vol. 70, no. 7, pp. 3052–3058, 1999.
- K. Heritage, C. Frisby, and A. Wolfenden, “Impulse excitation technique for dynamic flexural measurements at moderate temperature,” Review of Scientific Instruments, vol. 59, no. 6, pp. 973–974, 1988.
- R. M. Digilov, “Flexural vibration test of a cantilever beam with a force sensor: fast determination of Young's modulus,” European Journal of Physics, vol. 29, no. 3, p. 589, 2008.
- American Society for Testing and Materials, “Standard test method for dynamic Young’s modulus, Shear modulus, and poisson’s ratio for advanced ceramics by impulse excitation of vibration,” Standard C 1259-01, April 2001.
- Comité Européen de Normalisation, “Determination of dynamic elastic modulus by measuring the fundamental resonant frequency,” Standard EN 14146, 2004.
- D. J. Inman, Engineering Vibration, Prentice-Hall, Englewood Cliffs, NJ, USA, 1994.
- S. S. Rao, Mechanical Vibrations, Addison-Wesley, Menlo Park, Calif, USA, 3rd edition, 1995.
- K. R. Chun, “Free vibration of a beam with one end spring-hinged and the other free,” ASME Journal of Applied Mechanics, vol. 39, no. 4, pp. 1154–1155, 1972.
- “Multilab software for MultiLogPRO,” Fourier System, http://fourieredu.com/.
- Mathematica 7, Wolfram Research, Champaign, Ill, USA, 2008.
- J. R. Davis, Ed., Metals Handbook, ASM International, Materials Park, Ohio, USA, 1990.