1. Introduction
Lily, belonging to the family Liliaceae, is of edible and medicinal significance, exhibiting high nourishing effect and economic value [
1]. However, lilies are generally planted to a depth of 15–25 cm, causing soil disturbance during machine harvesting and increasing the chance of damage on lily bulbs [
2]. A numerical simulation study should be conducted on the mechanical harvesting process of lily bulbs to achieve high-efficiency and low-damage harvesting of lily bulbs and thus to provide a reference for the harvest mechanical design of lily bulbs. Before a numerical simulation study of the lily bulb is conducted, the intrinsic parameters of the lily bulb need to be determined [
3,
4,
5]. At the same time, the contact parameters between the lily bulb and the machine (Q235) need to be calibrated. The parameter calibration can be completed through a virtual simulation test and physical test.
At present, researchers around the world have conducted a significant amount of research on the model establishment and parameter calibration of agricultural bulk materials. Certain progress has been made in discrete element modeling and parameter calibration of related bulk materials, mainly including material grains, potatoes, animal manure, and soil particles [
6,
7,
8,
9,
10,
11]. Coetzee et al. [
12] employed the shear test and the confined compression test to complete the calibration of the friction coefficient and stiffness coefficient of the corn grains while performing physical test verification. Ghodki et al. [
13] established a soybean discrete element model and obtained the contact parameters of the model by comparing the characteristics of soybean shape and angle of repose. Ucgul et al. [
14,
15] achieved the calibration of soil cohesive force and non-cohesive soil simulation parameters by combining Hertz–Mindlin and Hysteretic spring contact models, and solved the problems of plastic deformation under stress. Hao Jianjun et al. [
16] built a discrete element model of Ma yam based on the accumulation of bimodal distribution. Shi Ronglin et al. [
17] designed a flax seed model based on the triaxial size of flax seeds and measured the physical parameters of three different flax seeds. Peng Caiwang et al. [
18] simulated the pile-up angle of the pig manure organic fertilizer particles treated with Heishui Fly through the steepest climbing test and the Box–Behnken test. Lu Fangyuan et al. [
19] calibrated the main contact parameters of the discrete elements of rice buds under different moisture contents depending on the experiment and simulation measurement of the friction angle of the rice buds. Research has demonstrated that it is feasible to obtain intrinsic parameters of bulk materials using the discrete element method. However, there is little research on the calibration of the discrete element model parameters for lily bulbs and machinery.
In sum, Longya lily planted in the Longhui area of Shaoyang, Hunan with a moisture content of 64.3% is used as a sample in this paper. Combined with bench tests and simulation tests, the establishment of the discrete element model of lily bulb was fulfilled using 3D reverse scanning to calibrate the contact parameters between the lily bulb and the machine (Q235 steel). Furthermore, the contact parameters between the lily bulbs were determined using a cylinder lifting, quadratic regression orthogonal rotation combination test, and response surface optimization methods. The pile-up angle test combining the physical test and the virtual test was conducted to verify the accuracy of lily bulb simulation parameters. There are two main innovations in this article. On the one hand, we established a discrete element model of lily bulb by using 3D reverse simulation engineering technology. On the other hand, we have verified the accuracy of the experimental values through a combination of virtual simulation experiments and physical experiments. Therefore, this research results can provide an accurate reference for the physical properties of lily in different stages, such as machine harvesting and postpartum processing.
2. Determination of Intrinsic Parameters of Lily Tubers and Establishment of Discrete Element Model
2.1. Triaxial Size Determination of Lily Tubers
According to the requirements of discrete element simulation, the basic physical parameters and contact parameters of the lily tubers need to be provided. The basic physical parameters include the triaxial size, mass density, elastic modulus, Poisson’s ratio, and moisture content of lily tubers. Contact mechanic parameters are composed of static friction coefficient, rolling friction coefficient, and collision recovery coefficient. Therefore, the triaxial dimensions of lily tubers should be determined first. In this study, the Longya lily planted in Longhui County, Shaoyang, Hunan Province was used as the research object. The five-point sampling method was used to sample Longya lily in Longhui County, Shaoyang to accurately establish a three-dimensional model of lily tubers. , 300 pieces were randomly selected, and a 111-101 type vernier caliper (precision 0.01 mm) was employed to measure their three-axis dimensions (maximum length L, maximum width W, maximum thickness T), the result being the averages collected. The three-axis size measurement of Longya Lily is illustrated in
Figure 1.
Table 1 presents the average values of maximum length L, maximum width W, and maximum thickness T of a Longya lily tuber obtained. Their values are 90.29, 81.43, and 65.27, respectively, with standard deviations of 0.438, 0.445, and 0.472. The overall shape of the tuber is ellipsoidal.
2.2. Moisture Content and Density
The moisture content of lily tubers was measured using the XF-110MA touch-type quick moisture meter (range 110 g). This instrument can be employed to automatically calculate the moisture content of materials according to their change quality. The water content of the lily tuber was measured after peeling off the lily tuber scales since the overall quality of a single lily tuber exceeded the maximum range of the instrument. During measurement, lily scales were put into the instrument and heated until moisture content became constant, and then its value was collected. The measurement was repeated 5 times to obtain the average value. The average moisture content of the lily tuber was calculated to be 64.3%.
DM-300, the density of lily tubers was measured using a density measuring instrument (range 0.01–300 g, accuracy 0.01 g). Similarly, a suitable number of lily scales was taken for density determination. This instrument can be adopted to automatically calculate the density of lily tubers by measuring the mass of lily scales and volume of drainage. Similarly, the experiment was repeated 5 times to acquire the average value. The density of the lily tuber was calculated to be 986 kg/m3.
2.3. Determination of Mechanical Characteristic Parameters of Lily
The stress state during the separation of fruit and soil should be analyzed to further establish its discrete element model, so as to ensure that the lily tubers are not damaged during the separation of fruit and soil during harvest. The HY-0580 microcomputer electronic universal testing machine was employed to measure mechanical characteristic parameters of lily bulbs through bending, compression, and shear tests.
2.3.1. Poisson’s Ratio
Lily tubers are too large in size and have thin and brittle skins and it is difficult to measure them directly with the general cylindrical sample compression method. Therefore, 10 lilies were randomly selected from the above samples, and lily scales with uniform texture were taken. Original dimensions of the lily scales in the width and the thickness directions were recorded. Hengyi HY-0580 universal material tensile and compression testing machine were taken to apply pressure (loading speed 0.1 mm/s) along with the width and thickness directions of the lily scale until it cracked. The universal material testing machine and an electronic vernier caliper were used to record the deformation in the width direction and the deformation in thickness of the lily at the limit of axial load cracking, respectively [
20]. Then, Poisson’s ratio of lily was calculated using Formula (1), and the average results were taken. The measured Poisson’s ratio of lily was 0.426.
where
μ denotes the Poisson’s ratio, indicates the deformation in the width direction of the lily scales, mm; represents the deformation in the thickness direction of the lily scales, mm;
W1 and
W2 designate the width of the lily scales before and after loading, respectively, mm;
T1 and
T2 refer to the thickness of the lily scales before and after loading, respectively, mm.
2.3.2. Elastic Modulus and Shear Modulus
Elastic modulus is a scale used to measure the ability of a material to resist elastic deformation. The elastic modulus must be measured first to calculate the shear modulus. In this test, 10 lilies were selected with scales taken off and uniform texture. Afterward, the A111-101 vernier caliper was used to measure their thickness before compression and then placed freely on the circle of the Hengyi HY-0580 universal material tensile and compression testing machine. On the platform, a circular indenter with a diameter of 5 mm was used. The speed before and during compression was 0.04 mm/s and 0.02 mm/s, respectively. The force (
F)-deformation (Δ
L) data was read and repeated for the selected 10 lilies. In the above test, the elastic and shear modulus of lily was calculated by Formulas (2) and (3):
where
E denotes the modulus of elasticity, MPa;
F refers to the axial load on the lily, N;
S is the contact area, mm
2, the diameter of the circular indenter is 5 mm, and the contact area with the lily scale is 11.465 mm
2; Δ
L indicates the lily scale subjected to the deformation after compression, mm;
L represents the thickness of the lily scale before compression, mm;
G is the shear modulus, MPa; designates the Poisson’s ratio of the lily scale. Through 10 measurements, the average value of lily’s elastic modulus was obtained to be 5.25 MPa, and the average value of the shear modulus is calculated to be 1.85 MPa.
2.4. Establishment of Discrete Element Model of Lily Bulb
A lily bulb is irregular in shape, and conventional modeling methods cannot accurately restore its true characteristics. In this paper, lily bulbs of moderate size (as shown in
Figure 2a) are selected as the research object to accurately establish a three-dimensional model of lily tubers and improve the authenticity of the simulation experiment. Furthermore, the three-dimensional scanning technology was applied, and an SP01-3D three-dimensional scanner (measurement accuracy 0.02 mm, scanning Range 10~1000 mm) was employed to scan the outer contour of the lily. Besides, 3D coordinates of the outer surface of the lily were accurately obtained to generate point cloud data and then exported to Geomagic Studio software (Geomagic Studio V2020, Rock Hill, NM, USA) for merging and splicing to obtain the lily model. Finally, the lily bulb model was imported into GOM Inspect (GOM Inspect, Braunschweig, Germany). The sharp and noisy points were sharpened using the software to obtain the three-dimensional lily model (
Figure 2b) [
21,
22,
23]. Next, the final lily 3D model was imported into EDEM2020 software (EDEM2020, Tory, USA) and filled with 149 spherical particles with radii ranging from 2–10 mm until the lily 3D model was tightly filled and there was no space to fill (
Figure 2c).
3. Calibration of Contact Parameters between Lily Bulb and Q235 Steel
In this paper, both bench and simulation tests are compared to calibrate the contact parameters of lily bulbs and Q235 steel and thus ensure the reference-ability of the discrete element simulation test. During the harvesting process, lily bulbs and Q235 steel material parts were in contact with each other. Additionally, the contact parameters between lily bulbs and Q235 steel and between lily bulbs are calibrated. Discrete element parameter calibration mainly adopted the collision bounce, inclined surface rolling, inclined surface slip, and accumulation tests. During the process of calibrating the contact parameters of lily bulbs and materials, the moisture content of lily bulbs had an essential influence on it. Therefore, lily bulbs with a moisture content of 64% after harvest were selected for the experiment. The simulation test parameters in EDEM software are exhibited in
Table 2.
3.1. Collision Recovery Coefficient
Collision recovery coefficient is a parameter of the ability of an object to recover after contact collision deformation. The collision recovery coefficient between lily bulbs and Q235 steel plate was calibrated by the collision bounce test [
25]. With the purpose of ensuring that lily bulbs do not break after being dropped and the bounce height is easy to distinguish, a preliminary test was conducted to reveal that the best height of lily bulbs to fall was 300 mm. As illustrated in
Figure 3a, the Q235 steel sheet was placed horizontally, and the lily bulb was freely dropped from the height h
1 of 300 mm. The lily bulb collides with the Q235 steel plate, and the highest bounce height of the lily bulb was recorded by high-speed video. This was repeated 5 times to obtain the average value (highest bounce height h
2 = 27.5 mm).
The static friction factor (x
2) and rolling friction factor (x
3) between lily bulbs and Q235 steel, as well as the collision recovery coefficient (X
1) and static friction factor (X
2) and rolling friction factor (X
3) between lily bulbs, have no effect on the bounce height. The values of x
2, x
3, X
1, X
2, and X
3 were all set to 0 to avoid interference in the EDEM simulation test. After pre-simulation tests, the range of the collision recovery coefficient x
1 of the lily bulb and Q235 steel was determined to be 0.20~0.40, and the step length was 0.04. There were 6 sets of simulation tests. Each set of tests were repeated 5 times to obtain the average value. The test design scheme and results are presented in
Table 3, in which y
1 denotes the simulation value of the highest bounce height of Q235 steel plate.
The curve fitting was performed on the test data in
Table 3 to obtain the relationship between the collision recovery coefficient of lily bulb–Q235 steel and lily bulb–clay soil and the maximum bounce height in the simulation test. The second-degree polynomial fitting curve was acquired, as presented in
Figure 4. The fitted curve equation (Equation (4)) is:
The determination system of Equation (4) was R2 = 0.981, which is close to 1, reflecting the high equation fitting reliability. The actual measured value of 27.5 mm of the lily bulb–Q235 steel plate was substituted into the Equation (4) to obtain x1 = 0.301, and input into the EDEM software for verification, repeated 5 times. Afterward, the average value was calculated. According to the test, the largest rebound height value was 26.24 mm, with a relative error value of 4.96%. The above comparison demonstrated that the simulation value was basically consistent with the bench test value. In the EDEM simulation test, the coefficient of recovery between the lily bulb and Q235 steel was determined to be x1 = 0.301.
3.2. Coefficient of Static Friction
The static friction factor is the ratio of the maximum static friction force experienced by the object to the normal pressure, and it can be examined by the inclined plane method. [
26] The static friction coefficient between the lily bulb and Q235 steel can be calibrated by the slope sliding method. The comparative test is exhibited in
Figure 5. In the beginning, Q235 steel plate was placed horizontally, and a lily bulb was placed on the Q235 steel plate. Thus, the Q235 steel plate rotated slowly and uniformly around one end. When the lily bulb started to slip, it stopped rotating. The frame test was repeated 5 times to acquire the average value. The measured value of the tilt angle of the inclined plate was
φ1 = 23.03°.
The rolling friction factor between lily bulbs and Q235 steel (x3), as well as the collision recovery coefficient (X1) and static friction factor (X2) and rolling friction factor (X3) of lily bulbs, had no effect on the tilt angle of the inclined plate. In the EDEM simulation test, the values of x3, X1, X2, and X3 were all set to 0 to avoid interference. The calibrated parameters were used in this research. The collision recovery coefficient between lily bulb and Q235 steel was x1 = 0.301. After the pre-simulation test, the static friction coefficient x2 between lily bulbs and Q235 steel in the range of 0.30~0.55, with a step length of 0.05, was used to conduct 6 sets of simulation tests. Each set of simulation tests were repeated 5 times to obtain the average value. The test design scheme and results are illustrated in the table, where y2 denotes the simulation value of the inclination angle of Q235 steel plate.
The curve fitting was performed on the test data in
Table 4 to acquire the relationship between the static friction factor and the inclination angle of the lily bulb and Q235 steel during the simulation test. The second-degree polynomial fitting curve was presented in
Figure 6. The curve equation (Equation (5)) is:
The coefficient of determination R2 of Equation (5) is 0.9887, which is close to 1, demonstrating the highly reliable fitting of the equation. Substituting the measured value of the inclination angle of the bench test (23.03°) into Equation (5), x2 = 0.423 was obtained and then input into EDEM for verification. The test was repeated 5 times to obtain the average value. The simulated value of the inclination angle measured by the simulation test was 22.05°; the error value between the simulated and measured values was 4.26%. The above comparison suggested that simulated and bench test values were the same. In the EDEM simulation test, the static friction factor x2 between the lily bulb and Q235 steel was determined to be 0.423.
3.3. Rolling Friction Factor
The rolling friction coefficient is a vital contact parameter between the lily bulb and Q235 steel. The inclined rolling test is mainly performed to calibrate the rolling friction coefficient between the lily bulb and Q235 steel. This test is illustrated in
Figure 7 [
27]. This test was conducted by placing the lily bulb on an inclined surface with an inclination angle of
φ2 = 40°, at a fixed height S
1 = 300 mm. Hence, the lily bulb rolls down the inclined surface with an initial speed of 0. The horizontal rolling distance of the lily bulb was measured when it rolled down and was completely still on the horizontal surface. The bench test was repeated 5 times to acquire the average value. The measured value of the horizontal rolling distance was S
2 = 149.8 mm.
The collision recovery coefficient between lily bulbs (X
1), static friction (X
2), and rolling friction (X
3) had no effect on the horizontal rolling distance. In the EDEM simulation test, the values of X
1, X
2, and X
3 were all set to 0 to avoid interference. The calibrated parameters were used in this research. The coefficient of recovery from the collision between lily bulb and Q235 steel was x
1 = 0.301 while the value of static friction was x
2 = 0.423. After the pre-simulation test, the rolling friction coefficient between lily bulb and Q235 steel x
3 was in the range of 0.04~0.09, with a step length of 0.01. Moreover, 6 sets of the simulation were conducted with each set of experiments repeated 5 times to take the average value. The experimental design plan and results are provided in
Table 5, where y
3 represents the simulation value of the horizontal rolling distance.
The curve fitting was performed on the test data in
Table 5 to obtain the relationship between the rolling friction factor and the horizontal rolling distance of the lily bulb and Q235 steel in the simulation test. The second-order polynomial fitting curve was obtained, as illustrated in
Figure 8. The curve equation (Equation (6)) y
3 is:
The coefficient of determination of Equation (6) was R2 = 0.9948, which was close to 1, indicating the high fitting reliability of the equation. By substituting the actual measured value of the horizontal rolling distance of 149.8 mm into Equation (6), x3 = 0.063 was obtained. This value was further entered into EDEM for verification. The test was repeated 5 times to obtain the average values. The simulated value of the horizontal rolling distance measured by the simulation test was 142.3 mm, with a measured relative error value of 5.3%, suggesting that the calibration simulation results are basically consistent with the bench test. In the EDEM simulation test, the coefficient of rolling friction between the lily bulb and Q235 steel was determined to be x3 = 0.063.