There is an increasing demand for a non-magnetic motor capable of rotation with high promotion torque at strong magnetic field of a super conduction, a medical care such as the MRI, and a magnetoence phalography. Because this non-magnetic motor does not have the adverse effects to a human body with an electromagnetic wave, the application to the healthcare setting is expected. The non-magnetic motors have been discussed quite a long time ago. Therefore, many studies have investigated the mechanisms of the motor using non-magnetic devices such as an electrostatic element [1] - [3] , an electrorheological fluid [4] , a shape memory alloy [5] , a magnetostrictive element [6] , and a combination of a frictional force and an electromagnetic force [7] [8] . As a masterpiece of the non-magnetic motor, an ultrasonic motor exists. Presently, the design and production technique of this ultrasonic motor are established. In addition, the ultrasonic motor is used for an electric appliance and a robot widely because the control characteristics are superior. However, this motor is very expensive although a cycle of the use is short.

In this paper, we propose a new non-magnetic motor of a stick type which combined the electrostatic force and mechanical resonance of a multilayer piezoelectric cantilever beam such as a bimorph cantilever beam. The bimorph cantilever beam with a silicon rubber piece was excited by using the electrostatic force. Then, the bimorph cantilever beam performs mechanical resonance, and the use of flexible material such as the silicon lubber enables conversion of translational vibration to rotary movement in one direction. In experiment, the rotational properties of the bimorph cantilever beam with the silicon rubber were examined firstly. Next, the stick type motor with two bimorph cantilever beams was fabricated, and the influence of each parameter on load torque and efficiency properties was considered.

Figure 1 shows a schematic diagram of a new motor of a stick type. The stick type motor consists of the bimorph cantilever beam, a flexible material such as the silicon rubber, a rotor, and a bearing. The bimorph cantilever beam with the silicon rubber performs resonance by an electrostatic force. The resonance energy rotates a rotor due to the frictional drive of the silicon rubber. The bimorph cantilever beam is composed of two piezoelectric ceramic trial pieces of 2 mm in width, 45 mm in length, and thickness 0.2 mm. A Ni alloy piece has 2 mm in width and 45 mm in length as shown in Figure 2. The silicon rubber of 2 mm in length, 0.5 mm in thickness, and 2 mm in width was used.

Table 1 shows material properties of the bimorph beam and the silicon rubber.

Figure 3 shows a placement of the silicon rubber piece and the rotor. The diameter of the rotor is 3 mm. The silicon rubber put off 0.5 mm from a center of the rotor. Furthermore, the silicon rubber and the rotor are contactless. Accordingly, the initial contact force between both does not occur.

By the choice of rigidity and dimensions of the silicon rubber, a design of the motor with a high output torque and low speed type, or a low output torque and high speed type is possible. This study considered balance of the high output torque and rotational speed. The dimensions of the silicon rubber made size of 2 mm in length, thickness 0.5 mm, and 1.5 mm in width as mentioned above. In this case, a spring constant K for bending of the silicon rubber is expressed as follows.

where, E is Young’s modulus, and I is the second section moments. From Equation (1), the spring constant K becomes 28.18 N/m. The motor of the high torque or the high rotational speed type can design freely by changing the spring constant. In future, it is necessary to check relationship between the rigidity of flexible materials and the output torque in detail. When the bimorph cantilever beam vibrates, the silicon rubber attached on the bimorph beam performs a translation motion and it contacts to the rotor. When the silicon rubber moves direction in coordinate x, tip of the silicon rubber will contact with a rotor, and it locks to the rotor as shown in Figure 4. Furthermore, by flexibility of the silicon rubber oneself, it transforms while locking to the rotor. The coefficient of friction between the silicon rubber and the rotor is μ, the imposition force by the silicon rubber is P, and a contact angle of the silicon rubber and the rotor is θ. By considering the moment at an arbitrary point A in the silicon rubber, the frictional force acting on tip of the silicon rubber by applying a result shown in previous paper [9] , as shown in Figure 5.

By Equation (2)

When is introduced here, Equation (3) is expressed as follows.

From the balance of the contact point of the silicon rubber and the rotor

From Equation (5)

Range in, the coefficient of friction becomes infinite from Equation (4). In this case, the silicon rubber is locking to the rotor, and transmits resonance energy to a rotor. The rotor rotates clockwise. On the other hand, when the bending deformation of the silicon rubber becomes large, the contact angle θ is small than. The lock of the silicon rubber is canceled. Accordingly, the silicon rubber gives resistance force of the sliding friction for a rotor. However, the rotor can rotate to one direction because a transmission force by the resonance energy is higher than frictional resistance.

The contact angle θ is approximately 37 degrees when the coefficient of friction between the silicon rubber and the rotor is 1.3 by using Equation (6). Accordingly, θ₁ is approximately 9 degrees by an initial position of the silicon rubber.

As shown in Figure 6, if the amplitude of the bimorph beam attached at position of the silicon rubber more than 1.15 mm, feed angle β per one period of the vibration by the silicon rubber becomes approximately 44 degrees by using Equation (7).

An experimental test was conducted using the apparatus shown in Figure 7. Firstly, the basic characteristic of the stick type motor was tested. In an experiment, by input into power amplifier a sine wave produced by the function generator, the bimorph cantilever beam vibrates in the resonance condition. The resonance frequency of first vibration mode measured by using experimental apparatus was 117 Hz and that of second vibration mode was 754 Hz. As a load torque, a commercially motor with small size was used. In an experiment, the load torque of the commercially motor was 19.6 μNm when no input current.

Figure 8 shows the relationship between an exciting frequency of the bimorph cantilever beam and rotational speed when the commercially motor was used as the rotor.

In this case, the input power was 0.018 W. The silicon rubber was attached to tip of the bimorph beam. The rotational speed increases in first and second resonance neighborhood.

Figure 9 shows the relationship between relative location ratio of the silicon rubber as shown in Figure 2 and rotational speed for first and second vibration mode of the bimorph cantilever beam when the input

power was 0.018 W. In this figure, and Δ indicate the experimental values for first and second vibration modes, respectively. When an attaching location ratio increases, the rotational speed increases for first vibration mode. However, for the second vibration, the attaching location ratio of no rotation by the influence of a nodal point occurs. When the attaching location ratio attached of the silicon rubber was 1 in both vibration modes, the rotational speed of the rotor becomes the maximum.

Figure 10 shows the relationship between the input voltage into the bimorph cantilever beam and rotational speed when the silicon rubber was attached at tip of cantilever beam. In this case, the rotational speed is proportional to the vibration amplitude linearly. The second vibration mode produces the high output by the small amplitude because resonance frequency of the second vibration mode is considerably high compared with first mode. The maximum rotational speed was 4200 rpm when the second mode was used.

Based on above result, the stick type motor with two bimorph cantilever beams was produced as shown in Figure 11. Figure 12 shows photograph of this motor. The motor has a length of 30 mm, a height of 6 mm, width of 5 mm, and total mass of 3 g. The diameter of the rotor is 3 mm and thickness is 3 mm. The diameter of an output axis for this motor is 0.3 mm. It is difficult to attach the output axis of the stick type motor into torque-meter. By using the commercial motor of diameter 6 mm, the output torque of the stick type motor was

indirectly measured by driving the commercial motor as load torque. About this commercial motor, relationship between an input electric current and output torque was measured before hand by using the torque meter as shown in Figure 13.

Figure 14 shows relationship between input current into the commercial motor and the output torque. When the electric currents increase, the torque increases linearly.

The output axis of the commercial motor was connected with the output axis of the stick type motor by using coupling component. The input electric current into the commercial motor was changed, and the output torque of the stick type motor was measured as shown in Figure 7. In this case, the commercial motor by applying the electric current was rotated to opposite direction compared with rotational direction of the stick type motor. Based on result of the measurement, the two bimorph cantilever beams were driven by second resonance frequency.

Figure 15 shows relationship between the output torque and rotational speed by changing the input power into the two bimorph cantilever beams. It is observed that this motor produces the output torque of 98 μNm when the rotational speed was 980 rpm.

Figure 16 shows relationship between the output torque and the efficiency when input power into the two bimorph cantilever beams was changed. The maximum efficiency was 24% when the input power was 0.065 W.

The section dimensions of the motor are considered, this motor produces high torque enough.

A new type of a non-magnetic motor which combined an electrostatic force and mechanical resonance was proposed and tested. Basic characteristics of the stick type motor with a bimorph cantilever beam, such as rotational speed, vibration modes, and installing positions of a silicon rubber were determined experimentally. The rotational speed of this motor increases the proportional with input voltage. The maximum rotational speed was 4200 rpm when an input voltage was set to 19 V.

Based on these results of a measurement, the stick type motor by two bimorph cantilever beams with the silicon rubber was produced. This motor produced the output torque of 98 μNm when the rotational speed was 980 rpm. The maximum efficiency was 24% when the input power was 0.065 W.

By coupling a lot of small cantilever beams, we are going to achieve improvement of the output torque in the future.

Hiroyuki Yaguchi, (2015) A New Motor of Stick Type with Coupled Mechanical Vibration of Bimorph Beam and Frictional Force. Engineering,07,446-454. doi: 10.4236/eng.2015.77040