# Method Improvements of Testing Modulus of Soil Based on Free-Vibration Column

Authors: Dandan Jin; Xianwen Huang; Binghui Wang; Aizhao Zhou; Shunqing Liu
Journal: Advances in Civil Engineering
 (2019)

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## Abstract

It is difficult to directly measure the dynamic elastic modulus of soils when the strain is less than 10−4, though the dynamic shear modulus can be easily obtained by the free-vibration testing method. Some improvements were adapted to the traditional free-vibration column for measuring dynamic elastic modulus of soil precisely with lateral vibration in small strain (10−4∼10−6). Differing from the traditional lateral vibration theory, a new dynamic elastic modulus testing method based on bending vibration equation of cantilever beam was put forward based on the improved free-vibration column of GZZ-50. Firstly, some descriptions about calibration process of needed testing parameter (moment of inertia of drive board) were made, and then, Poisson’s ratio of standardized column was used to confirm the measured results. Four main improvements were applied, including the shape of drive board which made the bending vibration equation solved, laser displacement sensors for correcting specimen’s height parameter with uncontacted manner which can reduce the influence of specimen, a hoop with plug used to make the split mould be removed, and air duct used when installing drive board to increase the success rate of installing specimen. Finally, standard process of installing specimen was described, which can be used as reference of similar test.


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## Body

## 1. Introduction

In recent years, more and more attention was paid to near-field earthquake, and the dynamic characteristic of soil under the effect of vertical earthquake was being more important in earthquake engineering. There are many indoor testing methods which were utilized to measure dynamic parameters of soil, such as the wave velocity method of bending element [1], resonant column [2] or free-vibration column testing method [3], dynamic triaxial testing method [4, 5], shear vibration testing method (torsion in the hollow column) [6, 7], and (centrifugal) shaking table test method [8, 9]. With the development of science and technology in testing instruments and increasing requirements of dynamic parameters of soil, testing instruments of dynamic characteristic of soil have been improving [10, 11]. Many new testing functions had been added [12], and more comprehensive testing theory had been put forward [13, 14].In soil dynamics and earthquake engineering, the dynamic shear and elastic modulus are the basic dynamic parameters of soil [15]. Dynamic triaxial test [16] is recognized as the most suitable instrument to measure the dynamic elastic modulus of soil, whose test results are reliable when the dynamic strain is between 10−4 and 10−2. But, the testing results are controversial when the strain is smaller than 10−4 due to the accuracy effect of testing instrument. When dynamic strain is smaller than 10−4, dynamic elastic or shear modulus of soil can be measured accurately by resonant (free-vibration) column in theory. The results of dynamic shear modulus measured by resonant (free-vibration) column with torsion in small strain is accepted by researchers [2, 3], and the testing process is simple, but the dynamic elastic modulus of soil is hard to be measured through axial vibrating of resonant (free-vibration) column, and less progress appears in this area decades.Cascante et al. [17] put forward a theory that the lateral vibration equation of cantilever beam can be used to measure the dynamic elastic modulus of soil simply. The lateral vibration of soil column was presumed as cubic polynomial equation, and the energy method and material mechanics were utilized to solve the frequency equation of bending vibration. Based on Cascabte’s method, Madhusudhan et al. [18] obtained the dynamic elastic modulus of Bangalore sand from lateral vibration tests. Analyzing the testing and solution process of the dynamic elastic modulus of Bangalore sand, the reasonability of some assumes is doubtful, such as the effect of bending moment of the drive board whether can be ignored and the vibration shape of soil column whether is reasonable. All of these will lead to deviation of testing results. In this paper, a new testing method to measure dynamic elastic modulus in presume that soil is elastic materials in small strain (<10−4) was put forward, whose reasonability had been proved [19]. The new method based on bending vibration equation [20] can consider the shear force and bending moment of the drive board well at the same time and remove the presume of cubic polynomial equation on vibration shape. Wang et al. [21] had discussed the solution process of this method and put forward that it can be applied to measure measuring dynamic elastic modulus of soil. But, they did not combine the corresponding instruments to describe the bending vibration equation detailed and did not explain the reasonability of some boundary conditions.Based on the above analysis, the article detailed the solution process of dynamic elastic modulus of soil column in terms of bending vibration equation and made four main improvements of traditional free-vibration column, which expands the testing scope of soil that cannot keep stability of the fixed shape in common confining pressure and improves the testing result quality of the specimen. The simple instruction of the instrument in this paper is shown in Figure1, (see the Appendix part of this paper). For better using improved GZZ-50 free-vibration column (made in china), the calibration process of the needed testing parameter (moment of inertia of the drive board) and the installation process of the specimen were detailed, and the deal processing of data was described briefly.Figure 1
Introduction of free-vibration column of GZZ-50.


## 2. Dynamic Elastic Modulus Testing Theory

### 2.1. Bending Vibration Equation

Cascante et al. [17] earlier put forward the appliance of lateral vibration test method in measuring the dynamic elastic modulus of soil. In analyzing, the vibration shape of soil column is assumed as cubic polynomial equation, and the additional force of drive board to the top of soil column is recognized as vertical shear force F. Then, material mechanics and energy method were used to solve the bending vibration equation. In Cascante’s method, there are two main purposes: Firstly, the vibration shape of soil column is defined as cubic polynomial equation, whose reliability is not sure. Secondly, when vibrating, the effect of drive board to the top of soil column is assumed as shear force, which ignores the effect of bending moment of the drive board. In real structure, the additional bending moment of the drive board is large, which has significant influence of the bending of soil column, and the influence will be more obvious with increasing strain. So, it is meaningful to find a more comprehensive method to calculate the dynamic elastic modulus of soil.Bending vibration equation of cantilever beam with additional mass is a good solution to calculate dynamic elastic modulus of uniform materials, and the corresponding calculating model is shown in Figure2. When calculating, the drive board is assumed as an additional mass attached at the top of beam, and the effect of additional mass to the top of soil column is recognized as shear force and bending moment according to the position of drive board (shown in Figure 3). For solving the frequency equation, some considerations were put forward including ① the strain of soil is in elastic period; ② some basic physical parameters of specimen are known or obtained, such as the diameter D, height L, mass m, and antibending stiffness EI; and ③ the mass and rotate inertia of the drive board mt and Jt have been measured or achieved.Figure 2
Vibration model of cantilever beam with additional mass.Figure 3
Model of lateral vibration with drive board.The microelement diagram of cantilever beam in lateral vibration is shown in Figure4. Rao [20] set up the bending vibration equation of cantilever beam with additional mass yx,t according to the force characteristic of cantilever beam with additional mass, which is shown in(1)EI∂4y∂x4+ρS∂2y∂t2=fx,t−∂∂xmx,t.Figure 4
Microelement diagram of cantilever beam.In actual testing, the exciting force which is arisen from the drive board makes the specimen obtain an initial strain in the specimen and then disappears quickly. After that, the specimen will vibrate in natural frequency and the vibrating amplitude will reduce gradually under the effect of damping. So, in solution process of free-vibration equation, the additional exciting force in function 1 is set as zero, and the free-vibration equation will be simplified to(2)∂2∂x2EI∂2yx,t∂x2+ρS∂2yx,t∂t2=0.


### 2.2. Solution of Dynamic Elastic Modulus

Function 2 can be solved using separation variable method and will be separated to(3)Yt=B1sinωt+B2cosωt,ϕx=A1cosβx+A2sinβx+A3chβx+A4shβx,where ω is the natural frequency, B1 and B2 are constants which can be confirmed according to initial situation, A1, A2, A3, and A4 are constants, which can be achieved from boundary conditions, and β can be repeated by β4=m¯ω2/EI where m¯ is mass per length of cantilever beam.Based on the boundary conditions from the fixed end of cantilever beam, function (4) can be obtained:(4)ϕx=0,ϕ′x=0.The function (5) can be achieved by combining function 3 and 4(5)A3=−A1,A4=−A2.When vibrating, the shear force which is arisen from the drive board can be represented asVL=−ω2ϕLmt, where mt is the mass of the drive board. Also, the bending moment which arises from rotation of the drive board can be represented as ML=−ω2ϕ′LJt+mtd02. Jt is the rotary mass moment of inertia of the drive board. The corresponding boundary conditions can be achieved in(6)EIϕ″L=−ω2ϕ′LJt+mtd02,EIϕ‴L=−ω2ϕLmt,where d0=0 can be obtained if the rotate axis of the drive board is set at the top of cantilever beam, which will be described in detail in Section 3.1. Combining functions (3), (5), and (6), function (7) can be obtained:(7)β2cosβL+chβL−ω2JtEIβsinβL+shβLβ2sinβL+shβL+ω2JtEIβcosβL−chβLβ3sinβL−shβL+ω2mtEIcosβL−chβL−β3cosβL+chβL+ω2mtEIsinβL−shβLA1A2=00.Function (7) is meaningful, and A1 and A2 are nonzero, so function (8) can be obtained:(8)β2cosβL+chβL−ω2JtEIβsinβL+shβL−β3cosβL+chβL+ω2mtEIsinβL−shβL−β2sinβL+shβL+ω2JtEIβcosβL−chβLβ3sinβL−shβL+ω2mtEIcosβL−chβL=0,where z≡βL and β4=m¯ω2/EI can be used to simplify function 8, and function 9 can be obtained:(9)αJαmz41−coszchz+αmzsinzchz−coszshz=αJz3sinzchz+coszshz+1+coszchz,where αJ=Jt/m¯L3=Jt/mL2 and αm=mt/m¯L=mt/m. αJ and αm are two dimensionless parameters which have concrete physical meaning. αJ is the rotate inertia ratio between the drive board and specimen column which can be obtained by calibrating and calculating (described in Section 2.1), and αm is the mass ratio between the drive board and specimen which can be obtained by weighting directly.It is hard to acquire the value ofz directly in function 9, for it is a transcendental equation. Hence, the numerical solution can be chosen to calculate the value of z. And then, the dynamic elastic modulus E can be achieved as shown in(10)E=mtω2L3z4I.


## 2.1. Bending Vibration Equation

Cascante et al. [17] earlier put forward the appliance of lateral vibration test method in measuring the dynamic elastic modulus of soil. In analyzing, the vibration shape of soil column is assumed as cubic polynomial equation, and the additional force of drive board to the top of soil column is recognized as vertical shear force F. Then, material mechanics and energy method were used to solve the bending vibration equation. In Cascante’s method, there are two main purposes: Firstly, the vibration shape of soil column is defined as cubic polynomial equation, whose reliability is not sure. Secondly, when vibrating, the effect of drive board to the top of soil column is assumed as shear force, which ignores the effect of bending moment of the drive board. In real structure, the additional bending moment of the drive board is large, which has significant influence of the bending of soil column, and the influence will be more obvious with increasing strain. So, it is meaningful to find a more comprehensive method to calculate the dynamic elastic modulus of soil.Bending vibration equation of cantilever beam with additional mass is a good solution to calculate dynamic elastic modulus of uniform materials, and the corresponding calculating model is shown in Figure2. When calculating, the drive board is assumed as an additional mass attached at the top of beam, and the effect of additional mass to the top of soil column is recognized as shear force and bending moment according to the position of drive board (shown in Figure 3). For solving the frequency equation, some considerations were put forward including ① the strain of soil is in elastic period; ② some basic physical parameters of specimen are known or obtained, such as the diameter D, height L, mass m, and antibending stiffness EI; and ③ the mass and rotate inertia of the drive board mt and Jt have been measured or achieved.Figure 2
Vibration model of cantilever beam with additional mass.Figure 3
Model of lateral vibration with drive board.The microelement diagram of cantilever beam in lateral vibration is shown in Figure4. Rao [20] set up the bending vibration equation of cantilever beam with additional mass yx,t according to the force characteristic of cantilever beam with additional mass, which is shown in(1)EI∂4y∂x4+ρS∂2y∂t2=fx,t−∂∂xmx,t.Figure 4
Microelement diagram of cantilever beam.In actual testing, the exciting force which is arisen from the drive board makes the specimen obtain an initial strain in the specimen and then disappears quickly. After that, the specimen will vibrate in natural frequency and the vibrating amplitude will reduce gradually under the effect of damping. So, in solution process of free-vibration equation, the additional exciting force in function 1 is set as zero, and the free-vibration equation will be simplified to(2)∂2∂x2EI∂2yx,t∂x2+ρS∂2yx,t∂t2=0.


## 2.2. Solution of Dynamic Elastic Modulus

Function 2 can be solved using separation variable method and will be separated to(3)Yt=B1sinωt+B2cosωt,ϕx=A1cosβx+A2sinβx+A3chβx+A4shβx,where ω is the natural frequency, B1 and B2 are constants which can be confirmed according to initial situation, A1, A2, A3, and A4 are constants, which can be achieved from boundary conditions, and β can be repeated by β4=m¯ω2/EI where m¯ is mass per length of cantilever beam.Based on the boundary conditions from the fixed end of cantilever beam, function (4) can be obtained:(4)ϕx=0,ϕ′x=0.The function (5) can be achieved by combining function 3 and 4(5)A3=−A1,A4=−A2.When vibrating, the shear force which is arisen from the drive board can be represented asVL=−ω2ϕLmt, where mt is the mass of the drive board. Also, the bending moment which arises from rotation of the drive board can be represented as ML=−ω2ϕ′LJt+mtd02. Jt is the rotary mass moment of inertia of the drive board. The corresponding boundary conditions can be achieved in(6)EIϕ″L=−ω2ϕ′LJt+mtd02,EIϕ‴L=−ω2ϕLmt,where d0=0 can be obtained if the rotate axis of the drive board is set at the top of cantilever beam, which will be described in detail in Section 3.1. Combining functions (3), (5), and (6), function (7) can be obtained:(7)β2cosβL+chβL−ω2JtEIβsinβL+shβLβ2sinβL+shβL+ω2JtEIβcosβL−chβLβ3sinβL−shβL+ω2mtEIcosβL−chβL−β3cosβL+chβL+ω2mtEIsinβL−shβLA1A2=00.Function (7) is meaningful, and A1 and A2 are nonzero, so function (8) can be obtained:(8)β2cosβL+chβL−ω2JtEIβsinβL+shβL−β3cosβL+chβL+ω2mtEIsinβL−shβL−β2sinβL+shβL+ω2JtEIβcosβL−chβLβ3sinβL−shβL+ω2mtEIcosβL−chβL=0,where z≡βL and β4=m¯ω2/EI can be used to simplify function 8, and function 9 can be obtained:(9)αJαmz41−coszchz+αmzsinzchz−coszshz=αJz3sinzchz+coszshz+1+coszchz,where αJ=Jt/m¯L3=Jt/mL2 and αm=mt/m¯L=mt/m. αJ and αm are two dimensionless parameters which have concrete physical meaning. αJ is the rotate inertia ratio between the drive board and specimen column which can be obtained by calibrating and calculating (described in Section 2.1), and αm is the mass ratio between the drive board and specimen which can be obtained by weighting directly.It is hard to acquire the value ofz directly in function 9, for it is a transcendental equation. Hence, the numerical solution can be chosen to calculate the value of z. And then, the dynamic elastic modulus E can be achieved as shown in(10)E=mtω2L3z4I.


## 3. The Calibration of System Parameters

### 3.1. Testing Process of Calibration

Before calibrating the testing parameters, some basic information about specimen is needed, including: the heightL, diameter D, mass m, and the mass of the drive board mt. The calibrating parameter Jt is hard to be measured directly for the complicated shape of drive board. When calibrating, more than 3 standard bars whose heights are different are needed, and they are made of identical materials and have the same section size, but the heights of them are different. The installed standard bar (shown in Figure 5) and concrete testing process are shown in the following:①
Make some measurements about needed parameters, including the height and mass of two standard barsL1, L2, m1, and m2 and the mass of drive board mt, and calculate the moment of inertia of the standard bar Ib.②
Separately conduct the tests of bending vibration of two standard bars. Then, the natural frequenciesω1 and ω2 of them can be obtained with the accelerometers according to different heights of standard bars.③
Solve function 9 which includes two unknown parametersJt and E in the method of combining two different equations, and the corresponding dynamic elastic modulus of standard bar E and rotational inertia of the drive board Jt can be obtained;④
Repeat the process ② and ③ and calculate theE and Jt many times to reduce the mistakes arisen from the data collection and calculation.⑤
Select different heights of standard bar, and repeat the above process.Jt can be corrected gradually to reduce the effect of standard bars’ height to the testing results.Figure 5
Photo of installed standard bar.


### 3.2. Checking with Standard Bar

After the rotational inertia of the drive boardJt is obtained, it is meaningful to check the measured results of free-vibration column. So, the standard bar consisted of elastic material, whose Poisson’ ratio is known can be used to check the measured results. The testing results are shown in Figures 6 and 7 separately.Figure 6
Test results of modulus.Figure 7
Test results of damping ratio.As is shown in Figure6, it can be found that dynamic shear modulus reduces less with the increase of dynamic strain. The average dynamic shear modulus is 75.84 GPa, and the difference between the maximum and minimum is 1.5%, which met the requirements of tests. The same changing tendency appears in the dynamic elastic modulus. The maximum dynamic elastic modulus 190.20 GPa appears at strain 2.35×10−6, the minimum value 187.92 GPa appears at strain 4.48×10−5, and the difference between them is 1.2% which met the requirements of tests. Based on the test results of elastic modulus, it can be found that the lateral vibration test has a good testing result in measuring the elastic modulus.Comparing the average dynamic elastic modulus and shear modulus, considering the Hooke’s law which describes the relationship between elastic modulus and shear modulus, Poisson’s ratio of materialμ can be obtained according to G=E/21+μ. Poisson’s ratio of the standard bar is 0.244, which is included in the period between 0.24 and 0.25. Poisson’s ratio of the standard bar can be obtained from manufacturers. Poisson’s ratio is connected with materials, which is easy to be obtained in real. So, it can be easily used to check the testing results.Figure7 shows the damping ratio and strain. It can be found that the damping ratio increases with the increasing of strain in lateral and shear vibrating tests, but the relative errors of damping ratio 0.85% and 0.68% are less than the requirements (2%). It means that the lateral and shear vibrating tests have a good result of the damping ratio by the improved instrument in this paper.


## 3.1. Testing Process of Calibration

Before calibrating the testing parameters, some basic information about specimen is needed, including: the heightL, diameter D, mass m, and the mass of the drive board mt. The calibrating parameter Jt is hard to be measured directly for the complicated shape of drive board. When calibrating, more than 3 standard bars whose heights are different are needed, and they are made of identical materials and have the same section size, but the heights of them are different. The installed standard bar (shown in Figure 5) and concrete testing process are shown in the following:①
Make some measurements about needed parameters, including the height and mass of two standard barsL1, L2, m1, and m2 and the mass of drive board mt, and calculate the moment of inertia of the standard bar Ib.②
Separately conduct the tests of bending vibration of two standard bars. Then, the natural frequenciesω1 and ω2 of them can be obtained with the accelerometers according to different heights of standard bars.③
Solve function 9 which includes two unknown parametersJt and E in the method of combining two different equations, and the corresponding dynamic elastic modulus of standard bar E and rotational inertia of the drive board Jt can be obtained;④
Repeat the process ② and ③ and calculate theE and Jt many times to reduce the mistakes arisen from the data collection and calculation.⑤
Select different heights of standard bar, and repeat the above process.Jt can be corrected gradually to reduce the effect of standard bars’ height to the testing results.Figure 5
Photo of installed standard bar.


## 3.2. Checking with Standard Bar

After the rotational inertia of the drive boardJt is obtained, it is meaningful to check the measured results of free-vibration column. So, the standard bar consisted of elastic material, whose Poisson’ ratio is known can be used to check the measured results. The testing results are shown in Figures 6 and 7 separately.Figure 6
Test results of modulus.Figure 7
Test results of damping ratio.As is shown in Figure6, it can be found that dynamic shear modulus reduces less with the increase of dynamic strain. The average dynamic shear modulus is 75.84 GPa, and the difference between the maximum and minimum is 1.5%, which met the requirements of tests. The same changing tendency appears in the dynamic elastic modulus. The maximum dynamic elastic modulus 190.20 GPa appears at strain 2.35×10−6, the minimum value 187.92 GPa appears at strain 4.48×10−5, and the difference between them is 1.2% which met the requirements of tests. Based on the test results of elastic modulus, it can be found that the lateral vibration test has a good testing result in measuring the elastic modulus.Comparing the average dynamic elastic modulus and shear modulus, considering the Hooke’s law which describes the relationship between elastic modulus and shear modulus, Poisson’s ratio of materialμ can be obtained according to G=E/21+μ. Poisson’s ratio of the standard bar is 0.244, which is included in the period between 0.24 and 0.25. Poisson’s ratio of the standard bar can be obtained from manufacturers. Poisson’s ratio is connected with materials, which is easy to be obtained in real. So, it can be easily used to check the testing results.Figure7 shows the damping ratio and strain. It can be found that the damping ratio increases with the increasing of strain in lateral and shear vibrating tests, but the relative errors of damping ratio 0.85% and 0.68% are less than the requirements (2%). It means that the lateral and shear vibrating tests have a good result of the damping ratio by the improved instrument in this paper.


## 4. Discussion about Improved Instrument

### 4.1. Adjustment of Drive Board Shape

As is shown in Figures8 and 9, it can be found that greater difference appears at the relative position of drive device (magnets) in the drive board. In traditional resonant column (shown in Figure 8), the drive device is set at the middle height of the drive board, which means that the mass center is in the middle of the drive board. In improved instrument, the drive device is set at the bottom height of the drive board, which means the mass center can be controlled at the bottom of the drive board in the method of attaching additional mass.Figure 8
Photo of traditional resonant column (copy from Madhusudhan and Senetakis [18]).Figure 9
Photo of free-vibration column of GZZ-50.When calculating the additional bending moment of the drive board, it is necessary to confirm the displacement between the drive board and the top of specimen column. The displacement reflects the value ofd0 in function 6. It is hard to measure the height of the mass center of the drive board to the top of specimen in traditional resonant column, but the problem can be solved well through the movement of the magnets’ position, which made the mass center be limited at the bottom of the drive board. So, the value of d0 in function 6 can be set as zero.


### 4.2. Installation of Laser Displacement Sensors

In experiments, the height of specimen will reduce during the necessary process of consolidation before vibrating; especially, the reduced height of specimen is more obvious when the specimen is soft soil. If we ignore it, then greater errors will appear. The effects of relative errors of specimen’s height to calculating results are shown in Table1:Table 1
The relative errors of height changes.
Relative errors of height (mm)
1
2
3
4
5
6
7
8
9
Calculation relative errors (%)
2.97
5.88
8.73
11.52
14.26
16.94
19.56
22.13
24.64As shown in Table1, due to the height changes of specimen, calculation relative errors will appear and increase rapidly with the increasing of measured height changes of specimen. When the relative error of height is 1 mm, the relative calculation errors will arrive at 2.97%, which is over the allowable error of tests (2%), and the calculation relative errors will increase rapidly with the increasing of height errors under the effect of cubed L in Function 10. So, it is significant to continuously confirm the height of specimen. In improved instruments, the laser displacement sensor was set above drive board, with a reflective face using a flat top screw installed at the center of the drive board (shown in Figure 10).Figure 10
Schematic diagram of process ⑤.Figure 11
Schematic diagram of process ①.


## 4.1. Adjustment of Drive Board Shape

As is shown in Figures8 and 9, it can be found that greater difference appears at the relative position of drive device (magnets) in the drive board. In traditional resonant column (shown in Figure 8), the drive device is set at the middle height of the drive board, which means that the mass center is in the middle of the drive board. In improved instrument, the drive device is set at the bottom height of the drive board, which means the mass center can be controlled at the bottom of the drive board in the method of attaching additional mass.Figure 8
Photo of traditional resonant column (copy from Madhusudhan and Senetakis [18]).Figure 9
Photo of free-vibration column of GZZ-50.When calculating the additional bending moment of the drive board, it is necessary to confirm the displacement between the drive board and the top of specimen column. The displacement reflects the value ofd0 in function 6. It is hard to measure the height of the mass center of the drive board to the top of specimen in traditional resonant column, but the problem can be solved well through the movement of the magnets’ position, which made the mass center be limited at the bottom of the drive board. So, the value of d0 in function 6 can be set as zero.


## 4.2. Installation of Laser Displacement Sensors

In experiments, the height of specimen will reduce during the necessary process of consolidation before vibrating; especially, the reduced height of specimen is more obvious when the specimen is soft soil. If we ignore it, then greater errors will appear. The effects of relative errors of specimen’s height to calculating results are shown in Table1:Table 1
The relative errors of height changes.
Relative errors of height (mm)
1
2
3
4
5
6
7
8
9
Calculation relative errors (%)
2.97
5.88
8.73
11.52
14.26
16.94
19.56
22.13
24.64As shown in Table1, due to the height changes of specimen, calculation relative errors will appear and increase rapidly with the increasing of measured height changes of specimen. When the relative error of height is 1 mm, the relative calculation errors will arrive at 2.97%, which is over the allowable error of tests (2%), and the calculation relative errors will increase rapidly with the increasing of height errors under the effect of cubed L in Function 10. So, it is significant to continuously confirm the height of specimen. In improved instruments, the laser displacement sensor was set above drive board, with a reflective face using a flat top screw installed at the center of the drive board (shown in Figure 10).Figure 10
Schematic diagram of process ⑤.Figure 11
Schematic diagram of process ①.


## 5. The Installation Process of Specimen

### 5.1. The Detailed Installation Process

For better application of improved resonant (free-vibration) column, authors described the installation process standardly, which is shown in the following steps:①
Soil column with height 100 mm and diameter 50 mm is prepared, and the weight of it has been measured. The prepared specimen should be kept constant. The filter paper should be put at the double end of soil column (shown in Figure11), which can not only avoid the block of water-permeable stone but also can reduce the partial destruction of stress arisen from the blade of the drive board when vibrating.②
Installation of the split mould is important for some low-strength soils which cannot retain the shape in natural pressure. The plug embeds the hoop with two circles, which can fix the split mould as shown in Figure12. The rubber diaphragm was turned down, and the rubber band was set.③
Set the drive board, connect the accelerometers, turn up the rubber diaphragm, move up the rubber band, and install the electromagnetic coil. It is important in this period that the blade of the drive board did not embed the soil.④
Push down the drive board vertically till the designed position and avoid rotating. The air focused on the top of specimen will remove along the hollow duct. After that, the hollow duct will be moved out.⑤
Set the two lines to the designed line ring which can be hooked when testing (shown in Figure10). Then, set confining pressure.⑥
Rotate the control bar to pull out the plug and open the split mould separately horizontally (shown in Figures10 and 13). Then, the installation of specimen has been finished.Figure 12
Schematic diagram of process ②.Figure 13
Schematic diagram of process ⑥.


### 5.2. Addition of Hoop with Plug

It is a bigger problem for resonant (free-vibration) column to measure the dynamic characteristic of soft soil, such as soft clay or loose sand. When testing, the specimen probably collapses under the gravity force of the drive board without effective confining pressure or the split mould supporting, which will lead to bad testing results or even failure of tests. Also, if the effective confining pressure exists, specimen can keep the original shape of the specimen without the split mould supporting in many cases. So, it is meaningful to remove the support of split mould without releasing the effective confining pressure in experiment.Hence, the hoop with plug (shown in Figure12) was added, which can simply make the split mould be removed without releasing confining pressure. The plug can be pulled out by the hook setting at the top of the device, and the constraint of split mould to the specimen will disappear. Then, the two split moulds will open (shown in Figure 13) under the effect of leash controlled by the hook too. The abovementioned device allowed the split mould to be removed under confining pressure, and owing to this improvement, the system expands the testing scope of soil types.


### 5.3. Addition of Air Duct

The contacting quality of the drive board to the soil column will have great influence to the testing results of specimen, but it is hard to guarantee in real installation. The contacting quality is closely related to the blade embed effect. When installing rubber diaphragm, rubber band, and other devices, it is significant to reduce disturbance of contacts between the drive board and specimen. In low-permeability materials, when the drive board was pushed down vertically, the air which is focused on void between the top of specimen and the drive board will be compressed. It will rebound the drive board after removing the push force, which will reduce the contacting quality seriously. So, the hollow duct can be used (shown in Figure14) to solve the problem through removing the air focused on the top of specimen. After installation, due to the effect of lubricating oil attached on the duct, the duct will be removed in low-disturbing level.Figure 14
Schematic diagram of processes ③ and ④.


## 5.1. The Detailed Installation Process

For better application of improved resonant (free-vibration) column, authors described the installation process standardly, which is shown in the following steps:①
Soil column with height 100 mm and diameter 50 mm is prepared, and the weight of it has been measured. The prepared specimen should be kept constant. The filter paper should be put at the double end of soil column (shown in Figure11), which can not only avoid the block of water-permeable stone but also can reduce the partial destruction of stress arisen from the blade of the drive board when vibrating.②
Installation of the split mould is important for some low-strength soils which cannot retain the shape in natural pressure. The plug embeds the hoop with two circles, which can fix the split mould as shown in Figure12. The rubber diaphragm was turned down, and the rubber band was set.③
Set the drive board, connect the accelerometers, turn up the rubber diaphragm, move up the rubber band, and install the electromagnetic coil. It is important in this period that the blade of the drive board did not embed the soil.④
Push down the drive board vertically till the designed position and avoid rotating. The air focused on the top of specimen will remove along the hollow duct. After that, the hollow duct will be moved out.⑤
Set the two lines to the designed line ring which can be hooked when testing (shown in Figure10). Then, set confining pressure.⑥
Rotate the control bar to pull out the plug and open the split mould separately horizontally (shown in Figures10 and 13). Then, the installation of specimen has been finished.Figure 12
Schematic diagram of process ②.Figure 13
Schematic diagram of process ⑥.


## 5.2. Addition of Hoop with Plug

It is a bigger problem for resonant (free-vibration) column to measure the dynamic characteristic of soft soil, such as soft clay or loose sand. When testing, the specimen probably collapses under the gravity force of the drive board without effective confining pressure or the split mould supporting, which will lead to bad testing results or even failure of tests. Also, if the effective confining pressure exists, specimen can keep the original shape of the specimen without the split mould supporting in many cases. So, it is meaningful to remove the support of split mould without releasing the effective confining pressure in experiment.Hence, the hoop with plug (shown in Figure12) was added, which can simply make the split mould be removed without releasing confining pressure. The plug can be pulled out by the hook setting at the top of the device, and the constraint of split mould to the specimen will disappear. Then, the two split moulds will open (shown in Figure 13) under the effect of leash controlled by the hook too. The abovementioned device allowed the split mould to be removed under confining pressure, and owing to this improvement, the system expands the testing scope of soil types.


## 5.3. Addition of Air Duct

The contacting quality of the drive board to the soil column will have great influence to the testing results of specimen, but it is hard to guarantee in real installation. The contacting quality is closely related to the blade embed effect. When installing rubber diaphragm, rubber band, and other devices, it is significant to reduce disturbance of contacts between the drive board and specimen. In low-permeability materials, when the drive board was pushed down vertically, the air which is focused on void between the top of specimen and the drive board will be compressed. It will rebound the drive board after removing the push force, which will reduce the contacting quality seriously. So, the hollow duct can be used (shown in Figure14) to solve the problem through removing the air focused on the top of specimen. After installation, due to the effect of lubricating oil attached on the duct, the duct will be removed in low-disturbing level.Figure 14
Schematic diagram of processes ③ and ④.


## 6. Testing Process and Data Deal

### 6.1. Testing Process

The functional division of free-vibration column of GZZ-50 is shown in Figure15. The testing process of lateral vibration includes the following after installation:①
Enter some basic physical parameters of specimen, including diameter, height, and the weight②
Calculatez in numerical method according function 9③
Start the lateral vibrating and record the data recorded by accelerometers④
Calculate dynamic elastic modulus based on the natural frequency and count the damping ratio in logarithmic function according to the curves of acceleration along time⑤
Increase amplitude of dynamic strain and repeat the above process till the tests are completed.Figure 15
Functional division of free-vibration column of GZZ-50: ① test type, ② data records of accelerometer, ③ exciting force of drive board, ④ results of Fourier transform, ⑤ date records of other information, ⑥ results of test, ⑦ test parameters, and ⑧ test controller.


### 6.2. Deal with Obtained Data

The testing results of soil are shown in Figure16. It can be found that the curves of testing results are not smooth, but the total tendency is clear. The greater measuring accuracy of accelerometer means many kinds of accelerate data will be recorded, which not only includes the natural accelerate of specimen but also includes the accelerate characteristic arisen from other situations, so the curves of accelerate is not single. The Fourier transform is a good solution for the problem [22]. The acceleration-time curves were transferred to amplitude-frequency curves (shown in Figure 17), and the natural frequency of specimen was obtained. Then, the dynamic elastic modulus of specimen will be obtained according to function 10, and the damping ratio will be obtained according to function 11:(11)λ=12π1mInAnAn+m,where An is the amplitude of nth peak and An+m is the amplitude of (n + m)’s peak.Figure 16
Curves of acceleration and time.Figure 17
Curves of amplitude and frequency.


## 6.1. Testing Process

The functional division of free-vibration column of GZZ-50 is shown in Figure15. The testing process of lateral vibration includes the following after installation:①
Enter some basic physical parameters of specimen, including diameter, height, and the weight②
Calculatez in numerical method according function 9③
Start the lateral vibrating and record the data recorded by accelerometers④
Calculate dynamic elastic modulus based on the natural frequency and count the damping ratio in logarithmic function according to the curves of acceleration along time⑤
Increase amplitude of dynamic strain and repeat the above process till the tests are completed.Figure 15
Functional division of free-vibration column of GZZ-50: ① test type, ② data records of accelerometer, ③ exciting force of drive board, ④ results of Fourier transform, ⑤ date records of other information, ⑥ results of test, ⑦ test parameters, and ⑧ test controller.


## 6.2. Deal with Obtained Data

The testing results of soil are shown in Figure16. It can be found that the curves of testing results are not smooth, but the total tendency is clear. The greater measuring accuracy of accelerometer means many kinds of accelerate data will be recorded, which not only includes the natural accelerate of specimen but also includes the accelerate characteristic arisen from other situations, so the curves of accelerate is not single. The Fourier transform is a good solution for the problem [22]. The acceleration-time curves were transferred to amplitude-frequency curves (shown in Figure 17), and the natural frequency of specimen was obtained. Then, the dynamic elastic modulus of specimen will be obtained according to function 10, and the damping ratio will be obtained according to function 11:(11)λ=12π1mInAnAn+m,where An is the amplitude of nth peak and An+m is the amplitude of (n + m)’s peak.Figure 16
Curves of acceleration and time.Figure 17
Curves of amplitude and frequency.


## 7. Conclusion

Based on analysis of the lateral vibration theory of cantilever beam with an additional mass and descriptions about improved free-vibration column of GZZ-50, the following conclusions can be obtained:(1)
According to bending vibration equation of cantilever beam with additional mass, linking with free-vibration column of GZZ-50, a new testing method to measure dynamic elastic modulus of specimen was put forward(2)
Making descriptions about the calibration process of system parameters, and applying standard bars to confirm the calibration results(3)
4 kinds of improvements of free-vibration column of GZZ-50 was proposed, including the adjustment of drive board shape, addition of hook with plug, laser displacement sensor uncontacted with specimen, and hollow duct, to improve the measured results or expand the testing scope of soil types(4)
The installation process of specimen and the deal process of data were described, which can be used as a reference of the similar instruments.



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*Source: 9743295-2019-10-31.xml*