# Effects of the Cone and Edge on the Acoustic Characteristics of a Cone Loudspeaker

Authors: Yue Hu; Xilu Zhao; Takao Yamaguchi; Manabu Sasajima; Tatsushi Sasanuma; Akira Hara
Journal: Advances in Acoustics and Vibration
 (2017)

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## Abstract

Loudspeakers are designed for reproducing the original sound field as faithfully as possible. In order to faithfully reproduce sound, it is important to understand the relationships among the physical characteristics of the loudspeaker. This paper focuses on the cone, the edge, and the behavior of air around the voice coil, which are important elements in the design of cone loudspeakers and evaluates their effects on the acoustic characteristics of the loudspeaker.


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## Body

## 1. Introduction

People hear a variety of sounds in their everyday lives. Loudspeakers are designed for faithfully reproducing the original sound field. Currently, the most commonly used loudspeaker design is the cone loudspeaker. For faithful sound reproduction, the relationships among the physical characteristics of the loudspeaker must be elucidated. One of the physical characteristics required for an ideal loudspeaker, assuming a constant input voltage, is a flat sound pressure in the frequency domain.In pursuit of this goal, researchers have long studied vibration analysis of the loudspeaker. Investigations of sound radiation by Brown [1] and Bordoni [2] treated the cone loudspeaker as a rigid body. However, the rigid body model of the cone is valid only during the so-called piston motion, in which the vibration system components, including the cone, edge, center cap, voice coil, and spider (see Figure 1), vibrate together as a unit in the low-frequency range. Nimura et al. [3] carried out a theoretical analysis of the vibration of the cone and used a graphical method to calculate the eigenvalues of the vibration of a conical loudspeaker cone. Kagawa [4] calculated the eigenvalues of the membrane vibrations of curved cones in addition to conical loudspeaker cones and found that curving the cone changed the eigenvalues of the membrane vibrations. Frankfort [5], also seeking solutions for the membrane vibrations of conical loudspeaker cones, formulated a differential equation that accounts for bending vibration and made detailed calculations of the sound pressure frequency response, vibration patterns, and driving-point admittance. However, Frankfort’s analysis did not account for the effects of the edge and center cap, which play important roles in cone loudspeakers. Subsequently, the finite element method (FEM) has been used for vibration analysis of the cone [6–11]. Kyouno et al. analyzed the sound radiation from loudspeakers, accounting for coupling of the electrical, mechanical, and acoustic systems [12].Figure 1
1/4 model of a loudspeaker.In these vibration analyses of cone loudspeakers, the cone maintains a piston motion in the low-frequency region. The biggest difficult point of these analyses is the split vibration of the vibration plate in the middle- and high-frequency regions. Control over the cone and the edge is very important in the design of a loudspeaker. However, there has been insufficient study of this topic in research up to now.Furthermore, these acoustic analyses, particularly in the case of FEM, do not account for air viscosity, which may reduce the accuracy of their estimates of sound pressure frequency properties.In particular, if the acoustic pathway in enclosure of small earphone is very narrow, air viscosity exerts a significant damping effect, reducing the estimation accuracy. Sasajima et al. succeeded at improving the estimation accuracy in the face of this problem by accounting for air viscosity using the finite element method [13].Loudspeakers larger than earphones have a narrow space between the voice coil and the magnetic circuit, making it very likely that air viscosity has a significant impact and is a factor of estimation errors of the sound pressure frequency. Therefore, general acoustic analyses need to account for the damping effect of air viscosity to accurately analyze loudspeakers.This paper examines cone loudspeakers, focusing intensively on the effects of the cone, the edge, and the narrow space between the voice coil and the magnetic circuit, which have a significant impact on the vibration characteristics and sound pressure frequency response. First, we perform an experimental study of the characteristics of a cone loudspeaker to determine its vibration characteristics and sound pressure frequency response. Next, we perform a vibration-acoustic analysis of the cone loudspeaker that accounts for the impact of air viscosity using our own independently developed acoustic analysis software. To verify the accuracy of our analysis, we compare the values from our analysis, which accounts for air viscosity, to the actual values of the vibration and sound pressure frequency properties. We also consider the behavior of the air around the voice coil. Finally, we calculate the optimal Young’s modulus and density of the cone and edge and examine in detail their impact on the vibration characteristics.


## 2. Methods and Materials

Figure1 illustrates the cone loudspeaker of diameter 0.16 m, which is the focus of this study. Because the cone exhibits axial symmetry, we assume a model that is 1/4 symmetric with respect to the x-z and y-z planes.The defining feature of cone loudspeakers is that the cone is approximately conical in shape, as illustrated in Figure1. The cone is supported by an edge around the outer periphery and a spider that supports the center of the cone by holding the voice coil in position. The outer perimeter of the spider is anchored to the frame. The cover at the center of the cone is typically a center cap, but our model used a whizzer cone to support the high-frequency characteristics.The voice coil is attached to the center of the cone, where it is supplied with the input signal current. These elements comprise the loudspeaker’s vibration system. The outer periphery of the vibration system is supported by a frame.The magnetic circuit for supplying magnetic flux to the voice coil consists of a plate, magnet, and yoke. Magnetic flux is supplied by the magnet through the yoke [14]. Sound waves are generated when the driving force generated according to Fleming’s left hand rule drives the cone, which is attached to the voice coil.A cross-sectional view of the cone loudspeaker is shown in Figure2. The performance of a loudspeaker is largely governed by its cone, which radiates the sound directly. In this sense, the cone can be said to be the heart of the loudspeaker. In an idealized model, the cone is always a rigid body travelling with a back-and-forth piston motion; however, in the middle- and high-frequency regions, the shape and material property values of the cone generate split vibrations in axisymmetric and nonaxisymmetric modes, exerting a significant influence on the loudspeaker’s vibration characteristics and sound pressure frequency response.Figure 2
Important elements of the design of cone loudspeakers.The edge, by undergoing large deformations and acting as a spring, not only facilitates movement of the cone in thez-axis direction but also plays a role in reducing movement in the x-y direction along the central axis. However, the edge does not always move back and forth together with the cone. The cone and the edge can vibrate in opposite phases, affecting the vibration characteristics.By controlling the characteristics of the cone and edge, which are important design elements of a cone loudspeaker, the vibration characteristics of the cone loudspeaker can be improved. This study examines the vibration characteristics of the loudspeaker by focusing attention on the materials of the cone and edge, which can be expected to have a particularly large impact.In addition, the narrow space between the outer perimeter of the yoke pole and the inner perimeter of the plate, indicated in Figure2, increases the air viscosity, and the flow of air in this gap can also be expected to have an important influence, which is very likely to be an error factor in the estimation of sound pressure frequency response. The damping effect of air viscosity, which is typically ignored in acoustic analysis, should therefore be taken into account for accurate analysis of loudspeaker performance.


## 3. Experimental

The performance of a cone loudspeaker is evaluated in terms of its vibration characteristics and sound pressure frequency properties; therefore, in our investigation, we took actual measurements of these characteristics.


### 3.1. Measurement of Cone Vibration Displacement

The cone is the core of a loudspeaker’s vibration system, and it is therefore very important to understand the vibration characteristics of the cone when designing a loudspeaker’s vibration system.We measured the cone’s vibration displacement using a laser displacement meter. Measurements were taken using a sweep signal of 10 Hz to 5 kHz, with the measurement point set to positionP at the center of the whizzer cone, which is located at the center of the loudspeaker cone (see Figure 2). The measurement system is shown in Figure 3.Figure 3
Cone vibration displacement measurement system.Figure4 shows the actual displacement characteristics at the measurement point. From 100 Hz to 800 Hz, the displacement can be seen to decrease nearly linearly; however, beyond 800 Hz, peaks occur at approximately 1 and 1.5 kHz.Figure 4
Comparison of the measurement result of cone vibration displacement amplitude.


### 3.2. Measurement of Sound Pressure Frequency Properties

We tested the sound pressure frequency of the loudspeaker by taking measurements in a reverberation room and an anechoic room, in accordance with the standards established in JIS Z 8732. Figure5(a) shows a schematic of the two-room measurement environment, with the reverberation room on the left and the anechoic room on the right. Figure 5(b) shows a photo of the reverberation room and anechoic room as seen from the outside. The insides of the reverberation room and anechoic room are shown in Figures 5(c) and 5(d), respectively.Figure 5
Measurement environment.
(a)
Schematic of measurement environment
(b)
Reverberation room and anechoic room
(c)
Reverberation room
(d)
Anechoic roomThe measurement system included an audio analyzer (Etani Electronics ASA-10 Mark II) and a microphone (Aco type 4012). The tests were performed using a sweep signal in the frequency range of 20 Hz to 20 kHz. The observation point for measurement of the sound pressure in the anechoic room was a position 0.8 m in front of the loudspeaker, on its central axis. The measurement system is shown in Figure6.Figure 6
Sound pressure frequency measurement system.The measurement results are shown in Figure7. An initial peak can be seen at approximately 80 Hz, and then the sound pressure frequency characteristic is generally flat from 200 Hz to 1 kHz. Above 1 kHz, a pattern of repeated peaks and dips can be observed.Figure 7
Comparison of measurement result and system characteristics of sound pressure frequency properties.We were able to determine the acoustic characteristics of the cone loudspeaker from the results of the measurements of the cone vibration displacement and the sound pressure frequency properties.However, these results by themselves do not reveal the impact of the cone and edge on the acoustic characteristics of the loudspeaker. This test was also inadequate in terms of the limited types of loudspeaker we were able to measure.Therefore, to elucidate the effect of the materials of the cone and edge on the acoustic properties of the loudspeaker, we continued our investigation as follows. First, we performed a coupled analysis of vibration and acoustics, taking air viscosity into account. Next, we compared the results of the analysis to the experimental values to verify the accuracy of the analysis. In lieu of an experiment, we used the acoustic analysis to reproduce the effects of the characteristics of the cone and edge on the acoustic characteristics of the loudspeaker. Finally, we applied the response surface methodology to determine the optimal cone and edge materials in order to design a loudspeaker with the desired acoustic characteristics.


## 3.1. Measurement of Cone Vibration Displacement

The cone is the core of a loudspeaker’s vibration system, and it is therefore very important to understand the vibration characteristics of the cone when designing a loudspeaker’s vibration system.We measured the cone’s vibration displacement using a laser displacement meter. Measurements were taken using a sweep signal of 10 Hz to 5 kHz, with the measurement point set to positionP at the center of the whizzer cone, which is located at the center of the loudspeaker cone (see Figure 2). The measurement system is shown in Figure 3.Figure 3
Cone vibration displacement measurement system.Figure4 shows the actual displacement characteristics at the measurement point. From 100 Hz to 800 Hz, the displacement can be seen to decrease nearly linearly; however, beyond 800 Hz, peaks occur at approximately 1 and 1.5 kHz.Figure 4
Comparison of the measurement result of cone vibration displacement amplitude.


## 3.2. Measurement of Sound Pressure Frequency Properties

We tested the sound pressure frequency of the loudspeaker by taking measurements in a reverberation room and an anechoic room, in accordance with the standards established in JIS Z 8732. Figure5(a) shows a schematic of the two-room measurement environment, with the reverberation room on the left and the anechoic room on the right. Figure 5(b) shows a photo of the reverberation room and anechoic room as seen from the outside. The insides of the reverberation room and anechoic room are shown in Figures 5(c) and 5(d), respectively.Figure 5
Measurement environment.
(a)
Schematic of measurement environment
(b)
Reverberation room and anechoic room
(c)
Reverberation room
(d)
Anechoic roomThe measurement system included an audio analyzer (Etani Electronics ASA-10 Mark II) and a microphone (Aco type 4012). The tests were performed using a sweep signal in the frequency range of 20 Hz to 20 kHz. The observation point for measurement of the sound pressure in the anechoic room was a position 0.8 m in front of the loudspeaker, on its central axis. The measurement system is shown in Figure6.Figure 6
Sound pressure frequency measurement system.The measurement results are shown in Figure7. An initial peak can be seen at approximately 80 Hz, and then the sound pressure frequency characteristic is generally flat from 200 Hz to 1 kHz. Above 1 kHz, a pattern of repeated peaks and dips can be observed.Figure 7
Comparison of measurement result and system characteristics of sound pressure frequency properties.We were able to determine the acoustic characteristics of the cone loudspeaker from the results of the measurements of the cone vibration displacement and the sound pressure frequency properties.However, these results by themselves do not reveal the impact of the cone and edge on the acoustic characteristics of the loudspeaker. This test was also inadequate in terms of the limited types of loudspeaker we were able to measure.Therefore, to elucidate the effect of the materials of the cone and edge on the acoustic properties of the loudspeaker, we continued our investigation as follows. First, we performed a coupled analysis of vibration and acoustics, taking air viscosity into account. Next, we compared the results of the analysis to the experimental values to verify the accuracy of the analysis. In lieu of an experiment, we used the acoustic analysis to reproduce the effects of the characteristics of the cone and edge on the acoustic characteristics of the loudspeaker. Finally, we applied the response surface methodology to determine the optimal cone and edge materials in order to design a loudspeaker with the desired acoustic characteristics.


## 4. Analysis and Results

In order to account for air viscosity, which is typically ignored in acoustic analyses of cone loudspeakers, we propose an application of the finite element method to perform a coupled analysis of vibration and acoustics that takes into account air viscosity.


### 4.1. Method of Analysis

As the acoustic element, consider a three-dimensional tetrahedral element with unknown nodal displacements, as illustrated in Figure8.Figure 8
Tetrahedral element.Lettingux, uy, and uz be the displacements in the x, y, and z directions, respectively, at any point in the element, the strain energy U~ can be expressed as follows:(1)U~=12E∭ve∂ux∂x+∂uy∂y+∂uz∂z2dxdydz.Here,E is the bulk modulus and ve is the volume of the tetrahedral element. Letting u˙ be the time derivative of the displacement, the kinetic energy T~ is expressed as follows:(2)T~=12∭veρu˙Tu˙dxdydz.Here,ρ represents the density of the element, and T represents the transposition. In addition, the viscous energy D~ of the viscous compressible fluid is expressed as follows:(3)D~=∭ve12T-TΓdxdydz.Here,{T-} is the stress vector due to viscosity, and Γ is the strain vector.Furthermore, using the potential energyV~ and applying Lagrange’s equation, we obtain an equation of motion for the air elements that accounts for air viscosity:(4)ddt∂T~∂u˙e-∂T~∂ue+∂U~∂ue-∂V~∂ue+∂D~∂u˙e=0.Here,ue and u˙e are the nodal displacement vector and nodal velocity vector, respectively. Substituting (1)–(3) into (4), the following equation is obtained:(5)-ω2Meue+Keue+Ceu˙e=fe.Here,Me, Ke, and Ce are the element mass matrix, the element stiffness matrix, and the element damping matrix, respectively. Furthermore, assuming a periodic response with an angular frequency of ω and using u˙e=jωue, (5) can be expressed by the following equation:(6)-ω2Meue+Keue+jωCeue=fe.Here,-ω2Meue is the inertia term, Keue is the stiffness term, jωCeue is the viscosity term, and fe is the external force.For the structural elements, we use the general formulation:(7)-ω2Mseuse+Kseuse=fse,where use, fse, Kse, and Mse are the structural elements’ nodal displacement vector, nodal force vector, complex stiffness matrix, and mass matrix, respectively. For the structural elements, in addition to tetrahedral elements, we also used hexahedral isoparametric elements account for incompatible modes.Superimposing these equations of motion on the elements in the places of interest and letting the displacements be the common unknown variables, the following equation of motion for the entire system, including structure and acoustics, is obtained:(8)-ω2Mu+Ku+jωCu=f.By solving the equation of motion in (8) for displacement, all nodal displacements can be determined. Furthermore, the strain and pressure of each element can be calculated from the nodal displacements [13].Therefore, we used solutions of (8) to carry out the coupled vibration and acoustic analysis described in this paper.To verify the performance of the loudspeaker, we relied primarily on frequency response analysis. To calculate the pressure of the elements during the actual vibration and acoustic analysis, we divided up the frequency range to be analyzed and then found the nodal displacementu corresponding to the sine wave excitation force f at each frequency. By repeating these calculations, the nodal displacement and element pressure were calculated for the entire frequency range to be analyzed, yielding frequency response characteristic graphs for displacement and pressure.


### 4.2. Analytical Model

We created an analytical model with conditions substantially equivalent to the conditions in the reverberation room and anechoic room shown in Figure5. As illustrated in Figure 9(b), the analytical model is composed of three parts: the sound-absorbing elements in the outer pink areas, the air elements in the inner green areas, and the cone loudspeaker setup in the airspace in the small reverberation room. Figure 9(a) shows the element model of the loudspeaker from the middle of Figure 9(b).Figure 9
Analytical model.Within the loudspeaker elements, there is a narrow width of only 2 × 10−5m between the voice coil and the magnetic circuit. In order to determine the behavior of the air around the voice coil in a way that accounts for the viscosity of the air, the fine air mesh shown in Figure 9(c) was created. For comparison, Figure 9(d) shows the state when there is no air between the voice coil and magnetic circuit.As a result, the structural part of the model contained 159,042 elements and 42,965 nodes, while the air part contained 704,942 elements and 143,585 nodes.The sine wave excitation forceF was applied to the entire circumference of the voice coil in the direction of the center axis of the loudspeaker, as shown in Figure 9(d).With respect to the boundary conditions, the three degrees of freedom on thex-, y-, and z-axes were fixed at the underside of the frame as shown in Figure 9(a) and at the exterior air nodes as shown in Figure 9(b). In addition, to account for symmetry conditions, the displacement of nodes on the y-z and x-z planes was fixed in the x-axis and y-axis directions, respectively.Since the loudspeaker is made of composite materials, the material properties used in our analysis were measured by the vibrating reed method [15] for the cone and whizzer cone, by the tensile test for the edge, and by FEM static analysis based on load displacement measurements for the spider. Other physical property values were obtained by consulting chronological scientific tables. Table 1 shows the actual physical property data used in our analysis. Other physical property values included an effective air density of 1.2 kg/m3, a bulk modulus of 1.4 × 105 N/m2, a coefficient of viscosity of 1.82 × 10−5 N·s/m2, and a speed of sound of 340.0 m/s.Table 1
Material and geometric parameters.
Parts
Mass density(kg/m3)
Young’s modulus(N/m2)
Poisson’s ratio
Cone
3.1 × 102
1.16 × 109
0.3
Edge
8.0 × 102
1.39 × 108
0.3
Spider
6.60 × 102
8.90 × 107
0.3
Whizzer cone
5.70 × 102
2.00 × 109
0.3
Voice coil
1.87 × 103
1.29 × 1011
0.34
Magnet
4.80 × 103
1.18 × 1011
0.3
Plate
7.69 × 103
2.00 × 1011
0.3
Yoke
7.94 × 103
2.00 × 1011
0.3
Frame
9.10 × 102
1.66 × 109
0.3


### 4.3. Verification of the Accuracy of Our Analysis of Cone Vibration Displacement

Figure10 shows a comparison of the cone vibration displacement amplitudes from the measurement results and analysis results. The solid line represents the measurement results, and the dashed line represents the results calculated by considering air viscosity.Figure 10
Comparison of the measurement result and analysis with viscosity of cone vibration displacement amplitude.The results in Figure10 show that the values from our analysis are in good agreement with the actual measured values. The fact that our calculation results yield roughly the same characteristics as the actual measured cone vibration displacement values suggests that highly accurate vibration analysis results can be obtained accounting for air viscosity.


### 4.4. Verification of the Accuracy of Our Analysis of Sound Pressure Frequency Properties

Figure11 compares the results of our calculation of the sound pressure frequency response in the direction of the axis of the loudspeaker to the actual measurement results from the sweep signal excitation. The solid line represents the measurement results, and the dashed line represents the results calculated by considering air viscosity.Figure 11
Comparison of measurement result and characteristics measurement system pressure frequency characteristics.The changes and characteristics of the sound pressure frequency response from our analysis results are consistent with the traditional view in the literature that more accurate characteristics can be obtained by analyses that account for the viscous damping of the air [16].The reason for this is that the narrow space between the voice coil and the magnetic circuit is so narrow that the air viscosity in the space affects the up-and-down motion of the voice coil. Our analysis is able to account for rotation as well as translational motion of air elements along thex-, y-, and z-axes. It is therefore able to represent the behavior of the air in the narrow passage, yielding calculation results that are closer to the actual measured values.


### 4.5. Impact of the Narrow Space between the Voice Coil and the Magnetic Circuit

When designing a cone loudspeaker, it is very important to consider the behavior of the air between the circumference of the voice coil and the magnetic circuit.Figure12(a) shows the behavior of the air around the voice coil when air viscosity is taken into account. Red indicates areas of large displacement and blue indicates areas of small displacement. When air viscosity is taken into account, the differences in air pressure become apparent, and, owing to the natural tendency of air to flow from areas of high pressure to areas of low pressure, the direction of the air flow from the vibration of the voice coil becomes apparent. Figure 12(b) shows the behavior of the air around the cone. The figure clearly shows the direction of the air flow around the cone due to the behavior of the air around the voice coil.Figure 12
Effect by vibration mode of air with viscosity.
(a)
Vibration mode around the voice coil
(b)
Vibration mode around the coneThe analysis results shown in Figure12 demonstrate the potential for consciously designing the fine-grained characteristics of a loudspeaker by adjusting parameters such as the viscous resistance of the narrow acoustic pathway between the voice coil and magnetic circuit.Using this analysis method, which accounts for air viscosity, it is possible to visualize the movement of air and capture the behavior of the air around the voice coil by solving the equation of motion with the nodal displacements as unknown quantities.


### 4.6. Impact of the Cone on the Acoustic Characteristics of the Loudspeaker

For purposes of comparison, we investigated cones made of both metal and paper-based materials. When metal is used, the material is highly uniform and exhibits greater flexural rigidity at the same thickness. On the other hand, when paper-based materials are used, the cone is easier to manufacture, but its vibration characteristics are likely to be more complicated because its flexural rigidity is lower than that of metal and the random arrangement of the pulp fibers renders the material nonuniform.Figure13 shows the cone displacement responses calculated by this method, accounting for air viscosity. The solid and dashed lines show the displacement responses for the metal and paper cones, respectively.Figure 13
Comparison vibration characteristic of metal cone and paper cone.The figure shows that the metal cone exhibits piston motion up to 5 kHz, with virtually no peaks and dips in displacement. In the case of the paper cone, more dips and peaks are observed, because the cone is softer and more prone to split vibration, in which the motion of the voice coil is not transmitted to the entire cone.


### 4.7. Impact of the Edge on the Acoustic Characteristics of the Loudspeaker

We compared the performance of an edge made of a soft material with Young’s modulus of 6.95 × 107 N/m2 and an edge made of a hard material with Young’s modulus of 2.78 × 108 N/m2. Figure 14 shows the vibration characteristics calculated by this method, taking into account air viscosity. The solid and dashed lines show the displacement response for the soft and hard materials, respectively.Figure 14
Comparison vibration characteristic of soft edge and hard edge material.The results in the figure show an initial peak at 1.3 kHz in the case of the soft edge material and an initial peak at 1.7 kHz in the case of the hard edge material. In other words, we used our analysis method to perform a coupled analysis of vibration and acoustics in which only the edge material was changed not the shape of the cone. These results demonstrate the potential for consciously designing the fine-grained characteristics of a loudspeaker, such as the first-peak position.


## 4.1. Method of Analysis

As the acoustic element, consider a three-dimensional tetrahedral element with unknown nodal displacements, as illustrated in Figure8.Figure 8
Tetrahedral element.Lettingux, uy, and uz be the displacements in the x, y, and z directions, respectively, at any point in the element, the strain energy U~ can be expressed as follows:(1)U~=12E∭ve∂ux∂x+∂uy∂y+∂uz∂z2dxdydz.Here,E is the bulk modulus and ve is the volume of the tetrahedral element. Letting u˙ be the time derivative of the displacement, the kinetic energy T~ is expressed as follows:(2)T~=12∭veρu˙Tu˙dxdydz.Here,ρ represents the density of the element, and T represents the transposition. In addition, the viscous energy D~ of the viscous compressible fluid is expressed as follows:(3)D~=∭ve12T-TΓdxdydz.Here,{T-} is the stress vector due to viscosity, and Γ is the strain vector.Furthermore, using the potential energyV~ and applying Lagrange’s equation, we obtain an equation of motion for the air elements that accounts for air viscosity:(4)ddt∂T~∂u˙e-∂T~∂ue+∂U~∂ue-∂V~∂ue+∂D~∂u˙e=0.Here,ue and u˙e are the nodal displacement vector and nodal velocity vector, respectively. Substituting (1)–(3) into (4), the following equation is obtained:(5)-ω2Meue+Keue+Ceu˙e=fe.Here,Me, Ke, and Ce are the element mass matrix, the element stiffness matrix, and the element damping matrix, respectively. Furthermore, assuming a periodic response with an angular frequency of ω and using u˙e=jωue, (5) can be expressed by the following equation:(6)-ω2Meue+Keue+jωCeue=fe.Here,-ω2Meue is the inertia term, Keue is the stiffness term, jωCeue is the viscosity term, and fe is the external force.For the structural elements, we use the general formulation:(7)-ω2Mseuse+Kseuse=fse,where use, fse, Kse, and Mse are the structural elements’ nodal displacement vector, nodal force vector, complex stiffness matrix, and mass matrix, respectively. For the structural elements, in addition to tetrahedral elements, we also used hexahedral isoparametric elements account for incompatible modes.Superimposing these equations of motion on the elements in the places of interest and letting the displacements be the common unknown variables, the following equation of motion for the entire system, including structure and acoustics, is obtained:(8)-ω2Mu+Ku+jωCu=f.By solving the equation of motion in (8) for displacement, all nodal displacements can be determined. Furthermore, the strain and pressure of each element can be calculated from the nodal displacements [13].Therefore, we used solutions of (8) to carry out the coupled vibration and acoustic analysis described in this paper.To verify the performance of the loudspeaker, we relied primarily on frequency response analysis. To calculate the pressure of the elements during the actual vibration and acoustic analysis, we divided up the frequency range to be analyzed and then found the nodal displacementu corresponding to the sine wave excitation force f at each frequency. By repeating these calculations, the nodal displacement and element pressure were calculated for the entire frequency range to be analyzed, yielding frequency response characteristic graphs for displacement and pressure.


## 4.2. Analytical Model

We created an analytical model with conditions substantially equivalent to the conditions in the reverberation room and anechoic room shown in Figure5. As illustrated in Figure 9(b), the analytical model is composed of three parts: the sound-absorbing elements in the outer pink areas, the air elements in the inner green areas, and the cone loudspeaker setup in the airspace in the small reverberation room. Figure 9(a) shows the element model of the loudspeaker from the middle of Figure 9(b).Figure 9
Analytical model.Within the loudspeaker elements, there is a narrow width of only 2 × 10−5m between the voice coil and the magnetic circuit. In order to determine the behavior of the air around the voice coil in a way that accounts for the viscosity of the air, the fine air mesh shown in Figure 9(c) was created. For comparison, Figure 9(d) shows the state when there is no air between the voice coil and magnetic circuit.As a result, the structural part of the model contained 159,042 elements and 42,965 nodes, while the air part contained 704,942 elements and 143,585 nodes.The sine wave excitation forceF was applied to the entire circumference of the voice coil in the direction of the center axis of the loudspeaker, as shown in Figure 9(d).With respect to the boundary conditions, the three degrees of freedom on thex-, y-, and z-axes were fixed at the underside of the frame as shown in Figure 9(a) and at the exterior air nodes as shown in Figure 9(b). In addition, to account for symmetry conditions, the displacement of nodes on the y-z and x-z planes was fixed in the x-axis and y-axis directions, respectively.Since the loudspeaker is made of composite materials, the material properties used in our analysis were measured by the vibrating reed method [15] for the cone and whizzer cone, by the tensile test for the edge, and by FEM static analysis based on load displacement measurements for the spider. Other physical property values were obtained by consulting chronological scientific tables. Table 1 shows the actual physical property data used in our analysis. Other physical property values included an effective air density of 1.2 kg/m3, a bulk modulus of 1.4 × 105 N/m2, a coefficient of viscosity of 1.82 × 10−5 N·s/m2, and a speed of sound of 340.0 m/s.Table 1
Material and geometric parameters.
Parts
Mass density(kg/m3)
Young’s modulus(N/m2)
Poisson’s ratio
Cone
3.1 × 102
1.16 × 109
0.3
Edge
8.0 × 102
1.39 × 108
0.3
Spider
6.60 × 102
8.90 × 107
0.3
Whizzer cone
5.70 × 102
2.00 × 109
0.3
Voice coil
1.87 × 103
1.29 × 1011
0.34
Magnet
4.80 × 103
1.18 × 1011
0.3
Plate
7.69 × 103
2.00 × 1011
0.3
Yoke
7.94 × 103
2.00 × 1011
0.3
Frame
9.10 × 102
1.66 × 109
0.3


## 4.3. Verification of the Accuracy of Our Analysis of Cone Vibration Displacement

Figure10 shows a comparison of the cone vibration displacement amplitudes from the measurement results and analysis results. The solid line represents the measurement results, and the dashed line represents the results calculated by considering air viscosity.Figure 10
Comparison of the measurement result and analysis with viscosity of cone vibration displacement amplitude.The results in Figure10 show that the values from our analysis are in good agreement with the actual measured values. The fact that our calculation results yield roughly the same characteristics as the actual measured cone vibration displacement values suggests that highly accurate vibration analysis results can be obtained accounting for air viscosity.


## 4.4. Verification of the Accuracy of Our Analysis of Sound Pressure Frequency Properties

Figure11 compares the results of our calculation of the sound pressure frequency response in the direction of the axis of the loudspeaker to the actual measurement results from the sweep signal excitation. The solid line represents the measurement results, and the dashed line represents the results calculated by considering air viscosity.Figure 11
Comparison of measurement result and characteristics measurement system pressure frequency characteristics.The changes and characteristics of the sound pressure frequency response from our analysis results are consistent with the traditional view in the literature that more accurate characteristics can be obtained by analyses that account for the viscous damping of the air [16].The reason for this is that the narrow space between the voice coil and the magnetic circuit is so narrow that the air viscosity in the space affects the up-and-down motion of the voice coil. Our analysis is able to account for rotation as well as translational motion of air elements along thex-, y-, and z-axes. It is therefore able to represent the behavior of the air in the narrow passage, yielding calculation results that are closer to the actual measured values.


## 4.5. Impact of the Narrow Space between the Voice Coil and the Magnetic Circuit

When designing a cone loudspeaker, it is very important to consider the behavior of the air between the circumference of the voice coil and the magnetic circuit.Figure12(a) shows the behavior of the air around the voice coil when air viscosity is taken into account. Red indicates areas of large displacement and blue indicates areas of small displacement. When air viscosity is taken into account, the differences in air pressure become apparent, and, owing to the natural tendency of air to flow from areas of high pressure to areas of low pressure, the direction of the air flow from the vibration of the voice coil becomes apparent. Figure 12(b) shows the behavior of the air around the cone. The figure clearly shows the direction of the air flow around the cone due to the behavior of the air around the voice coil.Figure 12
Effect by vibration mode of air with viscosity.
(a)
Vibration mode around the voice coil
(b)
Vibration mode around the coneThe analysis results shown in Figure12 demonstrate the potential for consciously designing the fine-grained characteristics of a loudspeaker by adjusting parameters such as the viscous resistance of the narrow acoustic pathway between the voice coil and magnetic circuit.Using this analysis method, which accounts for air viscosity, it is possible to visualize the movement of air and capture the behavior of the air around the voice coil by solving the equation of motion with the nodal displacements as unknown quantities.


## 4.6. Impact of the Cone on the Acoustic Characteristics of the Loudspeaker

For purposes of comparison, we investigated cones made of both metal and paper-based materials. When metal is used, the material is highly uniform and exhibits greater flexural rigidity at the same thickness. On the other hand, when paper-based materials are used, the cone is easier to manufacture, but its vibration characteristics are likely to be more complicated because its flexural rigidity is lower than that of metal and the random arrangement of the pulp fibers renders the material nonuniform.Figure13 shows the cone displacement responses calculated by this method, accounting for air viscosity. The solid and dashed lines show the displacement responses for the metal and paper cones, respectively.Figure 13
Comparison vibration characteristic of metal cone and paper cone.The figure shows that the metal cone exhibits piston motion up to 5 kHz, with virtually no peaks and dips in displacement. In the case of the paper cone, more dips and peaks are observed, because the cone is softer and more prone to split vibration, in which the motion of the voice coil is not transmitted to the entire cone.


## 4.7. Impact of the Edge on the Acoustic Characteristics of the Loudspeaker

We compared the performance of an edge made of a soft material with Young’s modulus of 6.95 × 107 N/m2 and an edge made of a hard material with Young’s modulus of 2.78 × 108 N/m2. Figure 14 shows the vibration characteristics calculated by this method, taking into account air viscosity. The solid and dashed lines show the displacement response for the soft and hard materials, respectively.Figure 14
Comparison vibration characteristic of soft edge and hard edge material.The results in the figure show an initial peak at 1.3 kHz in the case of the soft edge material and an initial peak at 1.7 kHz in the case of the hard edge material. In other words, we used our analysis method to perform a coupled analysis of vibration and acoustics in which only the edge material was changed not the shape of the cone. These results demonstrate the potential for consciously designing the fine-grained characteristics of a loudspeaker, such as the first-peak position.


## 5. Discussion

In the previous sections of this paper, we took into account the viscosity of the air, verified the accuracy of the coupled analysis of vibration and acoustics of the loudspeaker, and saw the impact of the material of the cone and edge on the acoustic characteristics of the loudspeaker. Extending this line of research, a significant remaining challenge is to design the appropriate cone and edge characteristics to obtain the desired acoustic characteristics in the loudspeaker.To address this challenge, in this section, we consider how to optimize the cone and edge, expressing the problem mathematically as follows:(9)Findx=ρc,Ec,ρe,EeTminW=fx=∑i=1ndi2i=1,2,…,nS.t.100kg/m3≤ρc≤1200kg/m37.3×108N/m2≤Ec≤70×108N/m2300kg/m3≤ρe≤1300kg/m33.2×107N/m2≤Ee≤20×107N/m2.Here,ρc is the density of the cone, Ec is Young’s modulus of the cone, ρe is the density of the edge, Ee is Young’s modulus of the edge, and W=f(x) is the objective function of optimization. In Figure 15, the solid line represents the target characteristic value, the dashed line (which was previously shown in Figure 10) represents the cone vibration displacement characteristics from our analysis, and di(i=1,2,…,n) represents the distance from the displacement characteristic to the target characteristic value at each frequency from 1 to 5 kHz. The number of sampling points was set to n=50.Figure 15
Cone vibration displacement amplitude standard analysis result and objective function.Although paper-based materials, metal materials, and other materials have been used to construct the sound-radiating cones in loudspeakers, paper-based materials are used most often. For that reason, the constraints imposed on the ranges of the cone’s density and Young’s modulus in (9) were set in the ranges for paper-based materials. Similarly, the range of values established for the edge in (9) reflects the fact that the edge is typically constructed using cotton fabric and rubber.We used the response surface methodology to optimize the physical properties of the cone and edge by carrying out the following calculation steps. First, we generated sample data in order to create the response surface for the optimization. Next, using the sample data, we carried out vibration analysis of the loudspeaker by changing the physical properties of each of its parts and, based on the results of the analysis, extracted the objective function values for the optimization calculation. Finally, we established a one-to-one correspondence between sample data and the characteristic values, created an interpolation approximation formula by the response surface method, and then used the approximation formula to find the optimum solution by performing the optimization calculation [17, 18].Table2 shows the sample data that was generated using the design variables and their upper and lower limit values, as well as the objective function value d, which is the result obtained from the coupled analysis of vibration and acoustics in accordance with the sample data.Table 2
Sample data and analysis results.
Number
Conemass density(kg/m3)
ConeYoung’s modulus(108 N/m2)
Edgemass density(kg/m3)
EdgeYoung’s modulus(107 N/m2)
Analysis resultsd
1
100
7.3
300
3.2
0.35
2
100
7.3
300
12
0.33
3
100
7.3
300
20
0.31
4
650
7.3
800
3.2
0.51
5
650
7.3
800
12
0.60
6
650
7.3
800
20
0.56
7
1200
7.3
1300
3.2
0.67
8
1200
7.3
1300
12
0.61
9
1200
7.3
1300
20
0.68
10
100
39
800
3.2
1.06
11
100
39
800
12
1.03
12
100
39
800
20
1.02
13
650
39
1300
3.2
1.29
14
650
39
1300
12
1.25
15
650
39
1300
20
1.27
16
1200
39
300
3.2
1.46
17
1200
39
300
12
1.43
18
1200
39
300
20
1.44
19
100
70
1300
3.2
0.98
20
100
70
1300
12
1.01
21
100
70
1300
20
1.00
22
650
70
300
3.2
1.55
23
650
70
300
12
1.56
24
650
70
300
20
1.55
25
1200
70
800
3.2
1.74
26
1200
70
800
12
1.77
27
1200
70
800
20
1.79We used these results to create the response surface and perform the optimization, the results of which are shown in Table3.Table 3
Design variables of optimization.
Initial value
Optimal value
ρ
c (kg/m3)
650
100
E
c (N/m2)
39 × 108
28 × 108
ρ
e (kg/m3)
800
800
E
e (N/m2)
12 × 107
20 × 107Figure16 shows the results of the vibration analysis using the optimal solution that was obtained. The black solid line represents the analysis result for the optimal solution and the red solid line represents the target characteristic values. The dashed line represents analysis results for the original loudspeaker shown in Figure 10. The results obtained for the optimal solution closely match the target characteristic values.Figure 16
Analysis result of optimal solution.The optimal solution exhibits flatter characteristics compared to the original cone vibration displacement characteristics, which exhibited peaks at 1.5 and 3 kHz and a dip at 2.5 kHz. The characteristics also appear flatter over the entire frequency range. The result of the objective function valued for the optimal solution was d=0.26, which represents an improvement of approximately 35% over the original loudspeaker, for which the result was d=0.40.In the optimal solution, the density of the cone was 100 kg/m3, and Young’s modulus was 28 × 108 N/m2. These properties define a cone that is lighter in weight and vibrates more easily but whose stiffness enables suppression of split vibration in the nonaxisymmetric mode. This suggests that cones should be constructed from light but rigid materials.The results for the edge were a density of 800 kg/m3 and Young’s modulus of 20 × 107 N/m2. Since the edge supports the cone, this suggests that edges should be constructed of materials with high rigidity.In addition, the vibration mode of the cone was examined. The vibration modes of the cones are shown in Figure17. Red and blue indicate areas of large and small displacement, respectively. Figure 17(a) shows the vibration mode of a standard loudspeaker cone at 1.5 kHz, and Figure 17(b) shows the vibration displacement mode of an optimal cone at 1.5 kHz. In the case of the standard loudspeaker, it can be seen that the displacement is smaller at the center of the cone and greater at the periphery (the part attached to the edge), whereas the optimal cone moves with the same amount of displacement.Figure 17
Analysis result of optimal solution: cone A at 1500 Hz.
(a)
Vibration mode of the standard cone
(b)
Vibration mode of the optimal coneBy changing Young’s modulus and density of the cone and edge, we were able to reduce the peaks that occur due to split vibration of the cone in the middle- and high-frequency regions above 1 kHz and achieve flatter frequency characteristics.


## 6. Conclusion

This study focused on the cone, the edge, and the behavior of air around the voice coil, which are important elements in the design of cone loudspeakers, and evaluated their effects on the acoustic characteristics of a loudspeaker. We performed a coupled analysis of the vibration and acoustics of a cone loudspeaker that accounted for the impact of air viscosity, which has received little attention in traditional acoustic analyses, and then sought optimal materials for the cone and edge. The following results were obtained:(1)
We took measurements of the vibration characteristics and sound pressure frequency response of a cone loudspeaker in order to determine its acoustic characteristics.(2)
We performed a coupled analysis of the vibration and acoustics of the loudspeaker that accounted for air viscosity and compared the vibration characteristics and sound pressure frequency response to the actual measured values. By accounting for air viscosity, the analysis was able to yield high accuracy.(3)
The coupled analysis of vibration and acoustics revealed the vibration characteristics of the cone, which are influenced by the characteristics of the cone and edge. Furthermore, with respect to the behavior of the air around the voice coil in the loudspeaker, the results of our analysis, which accounted for air viscosity, enabled us to clearly see the direction of air movement; this is not possible with traditional analyses. This led to an improvement in the accuracy of the analysis.(4)
We used the response surface methodology to optimize the design of Young’s modulus and density of the cone and edge and obtained the optimum physical properties of the cone and edge in order to design a loudspeaker with the desired acoustic characteristics. The optimal solution that was obtained reduced the peaks and dips caused by split vibration of the cone and achieved flatter vibration characteristics.With respect to future challenges, we hope to investigate the analysis of loudspeakers of complex shapes, beyond typical cone loudspeakers. In addition, we would like to alter the shape of the loudspeaker components in ways that will lead to an optimum design to achieve flatter sound pressure frequency properties.



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*Source: 2792376-2017-05-21.xml*