Abstract
Combined with the transmission mode of cycloid permanent magnet gear and ring plate mechanical gear, a three-shaft ring-plate permanent magnet gear transmission structure (TRMG) is proposed. Operating mechanism of structure is given. TRMG simulation model is established and the correctness is verified by transient finite element method. Based on momentum moment theorem, TRMG start-up process and start-up position of are analyzed theoretically. By calculating TRMG torque impulse, the optimal start-up range and start-up position of TRMG are determined.
Keywords: Multi-axle ring-plate permanent magnet gear, Start-up characteristics; Start-up position, Dynamic characteristics
1. Introduction
Start-up characteristics refer to the dynamic characteristics of driven rotor at rated load condition from stationary to stable operation stage. Mechanical gearbox, as an important core component of electromechanical transmission system, bears a large impact load in start-up process. With the increase of service frequency, a series of faults such as oil leakage, shaft channeling and tooth damage often occur in mechanical gearbox [1,2].
The non-contact transmission of permanent magnet gear using air gap magnetic field solve the damage caused by starting process of mechanical gear, and realize the conversion requirements between low speed and high speed and low torque which has a broad application prospect [3-5].
Literature [6] based on the principle of mechanical Cycloid Gear transmission, a transmission structure of Cycloid permanent Magnetic Gear, CMG is proposed, which has high transmission ratio and high torque density (Transmission ratio≥20, Torque density≥180kNm/m3). Since then, scholars have studied the transmission structure, magnetization, bearing capacity and eddy current loss of CMG, and further improved the transmission ratio and torque density of structure (Transmission ratio≥100, Torque density≥280kNm/m3) [7-10].
Although CMG has large transmission ratio and torque density, its service life is relatively short due to a large unbalanced magnetic pull by internal rotor shaft. In addition, the start-up characteristics of CMG have not been studied in the above literatures [11,12].
In order to improve the service life of CMG rotating arm bearing and solve start-up characteristics, this paper proposes a three-shaft ring-plate permanent magnet gear transmission structure (TRMG) based on ring-plate mechanical gear transmission mode. Compared with CMG, TRMG moves the rotating arm bearing to the outside of the cycloid wheel to increase the number of rotating arm bearing, disperse the payload of rotating arm bearing and prolong the service life of rotating arm bearing. In addition, this paper uses theorem of momentum moment to analyze the start-up position of TRMG and determine the optimal start-up range and start-up position of TRMG.
2. TRMG Operation mechanism
Figure 1 shows the mechanical structure of TRMG. In Figure 1, three eccentric high-speed shafts are connected with ring plate permanent magnet ring through rotating arm bearings. The ring plate permanent magnet ring consists of outer yoke iron and outer ring permanent magnet, and is located outside the low-speed permanent magnet ring. The low-speed permanent magnet ring is composed of inner yoke iron and inner ring permanent magnet, and a low-speed shaft is installed in the center.
In Figure 1, the center distances of three eccentric high-speed shafts to low-speed shaft are equal to the eccentricity between ring plate permanent magnet ring and low-speed permanent magnet ring. The low-speed permanent magnet ring rotates around the center of low-speed shaft.
When the eccentric high-speed shaft moves the ring plate permanent magnet ring, the outer ring permanent magnet revolves around the inner ring permanent magnet. As the relative position of two permanent magnets changes, the permanent magnet embedded in low-speed permanent magnet ring is driven to rotate low-speed shaft by the change of magnetic field force.
Due to the large difference between the eccentricity and the radius of the low-speed permanent magnet ring, a large transmission ratio can be achieved.
Set transmission ratio of TRMG as Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle i}
, and pole pairs of inner ring permanent magnet and outer ring permanent magnet as Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle p_\mbox{i}}
and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle p_\mbox{o}}
respectively, then:
|
(1) |
Since the pole pairs of outer ring permanent magnet is always one more than that of inner ring permanent magnet, when the ring plate permanent magnet ring revolves around the low-speed permanent magnet ring once, the low-speed permanent magnet ring rotates a pair of magnetic poles in reverse.
3. TRMG start-up position analysis
Set the eccentric high-speed shaft be driving shaft (the active motion of ring plate permanent magnet ring), and the low-speed shaft be driven shaft (the connection load of low-speed permanent magnet ring), and the starting angle between ring plate permanent magnet ring and low-speed permanent magnet ring is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta }
, and the output torque of low-speed permanent magnet ring is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): M_{out}
. It can be seen from literature [13-15] that:
|
(1) |
In Equation (1), Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): M_{max}
is the static maximum torque. Figure 2 shows the relationship between Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): M_{out}
and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta }
.
In Figure 2, when starting angle is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_1}
, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_3}
, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_6}
or Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_7}
the output torque of point Q, V, K or Z is equal to the load torque Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): M_{load}
. When the starting angle is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_2}
, the output torque of point U is the static maximum torque Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): M_{max}
. When the starting angle is 0, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_4}
or Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_5}
, the structures of point P, W or I are in start-up equilibrium position.
Set the difference between output torque and load torque as Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta M}
, then:
|
(2) |
|
(3) |
|
(4) |
In Equations (3) and (4), Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): J
is the inertia of low-speed permanent magnet ring; Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): \sigma
is its angular velocity; Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): \Delta \sigma
is the change of angular velocity.
When the relative rotation angle between the ring plate permanent magnet ring and the low-speed permanent magnet ring increases from 0 to Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_1}
, set the work done by Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta M}
on the rotor be Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle G_1}
, then:
|
(6) |
Substituting Equations (3) and (4) into Equation (6), and the equation (6) is transformed by equality, we can get:
|
(7) |
It can be seen from Figure 2 that the first integral in Equation (7) can be approximately regarded as the area of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
. When TRMG runs at curve PQ, the forward electromagnetic torque of low-speed permanent magnet ring is less than load torque, and the reverse acceleration can be obtained. Therefore, Equation (7) can be written as:
|
(8) |
Equation (8) can be simplified as follows:
|
(9) |
In Equation (9), TRMG starts from static state, so Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\sigma }_0\mbox{=}0
.
According to Equation (9), if Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
is larger, the reverse acceleration kinetic energy and reverse impulse obtained by low-speed permanent magnet ring are larger at this stage, and TRMG is more difficult to start, so it is called deceleration area.
Similarly, when the relative angle between the ring-plate permanent magnet ring and the low-speed permanent magnet ring increases from Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_1}
to Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_3}
, set the work done by Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_3}
on rotor be Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle G_2}
, then:
|
(10) |
The integral of first term in Equation (10) can be approximated as Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{QUV}}
area. As TRMG runs at curve QV, the forward electromagnetic torque received by low-speed permanent magnet ring is greater than load torque, and the forward acceleration can be obtained. Therefore, Equation (10) can be expressed as:
|
(11) |
Equation (11) can be simplified as follows:
|
(12) |
According to Equation (12), if Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{QUV}}
is larger, the forward acceleration kinetic energy and forward torque impulse obtained by rotor can more easily offset the reverse impulse when Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta \in [0,{\beta }_1]}
, and TRMG can more easily start-up, so it is called acceleration area.
4. TRMG start-up process analysis
Set the relative rotation angle of ring plate permanent magnet ring and low-speed permanent magnet ring is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha }
.
According to the operation mechanism of TRMG, due to TRMG is in equilibrium position before start-up, the output torque of TRMG is 0 as the force between air gap magnetic fields of the ring plate permanent magnet ring and the low-speed permanent magnet ring is balanced. At this point, the equilibrium position of TRMG can be divided into two kinds: one is that when TRMG is start-up, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle M}
increases positively with Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha }
increase; The other is that when TRMG is start-up, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle M}
reverse increases with α increase.
Set the starting point of TRMG Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left(\beta =0\right)}
is started at equilibrium position of forward torque period, and the active rotor is generated a forward rotating magnetic field by the action of magnetic field air gap.
When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [0,{\beta }_1]}
, there is a slip between ring plate permanent magnet ring and low-speed permanent magnet ring, and the forward electromagnetic torque of low-speed permanent magnet ring is less than load torque, the low-speed permanent magnet ring speeds up in reverse rotation and generates a reverse impulse of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
. TRMG does not start properly at this stage.
When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_1,{\beta }_3]}
, the electromagnetic torque of low-speed permanent magnet ring is always larger than load torque, and the forward angular acceleration can be obtained and the forward impulse of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{QUV}}
can be generated. Since the low-speed permanent magnet ring has acquired the reverse impulse of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
to accelerate in reverse, the low-speed permanent magnet ring decelerates in reverse and then accelerate in forward direction by the action of forward torque impulse.
If Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}<\Delta \mbox{QUV}}
, before Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha }
increases to Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle {\beta }_3}
, the low-speed permanent magnet ring reaches synchronous speed of rotating magnetic field, and TRMG enters adjustment stage of speed and torque. By combined action of magnetic and mechanical damping, TRMG oscillation gradually attenuates, and the rotational speed and torque gradually become stable.
If Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}>\Delta \mbox{QUV}}
, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha }
enters interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_3,{\beta }_4\right]}
, the forward electromagnetic torque of low-speed permanent magnet ring is less than load torque, which makes it decelerate forward first and then accelerate backward. Due to the speed of low-speed permanent magnet ring is still less than synchronous speed of rotating magnetic field, and TRMG accelerates in reverse by combined action of reverse electromagnetic torque and load torque, which eventually leads to start-up failure.
The above analysis shows that:
(1) If TRMG start-up smoothly, the low-speed permanent magnet ring should reach synchronous speed by sufficient forward electromagnetic torque impulse in Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[0,{\beta }_4\right]}
interval.
(2) If Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{QUV}}
(acceleration area) remains same, adjust Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta }
to reduce Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
(deceleration area), so as to reduce the reverse torque impulse of low-speed permanent magnet ring, easy to start-up.
When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta \in [{\beta }_1,{\beta }_2]}
, TRMG can start-up normally. When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta \in [0,{\beta }_1]\cup [{\beta }_2,{\beta }_3]}
, TRMG may not start-up. When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta \in [{\beta }_3,{\beta }_4]}
, TRMG cannot start-up, so the start-up position determines whether TRMG starts smoothly.
5. TRMG finite element simulation analysis
Due to ANSYS Maxwell simulation software cannot dynamically simulate the object rotating around eccentric axis, in order to verify the start-up position theory, TRMG should be equivalent to a model, and the operation process of TRMG can be judged by verifying the dynamic characteristics of the equivalent model.
5.1 Dynamic characteristics of TRMG equivalent model
Set TRMG transfer power Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle P=1\mbox{kw}}
, output speed Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle n_\mbox{o}\mbox{=}67\mbox{r/}min}
, transmission ratio Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle G=22:1}
, TRMG structure parameters as shown in Table 1 can be obtained.
| Symbol | Description | Value (Unit) | |
| pi | Pole pairs of inner permanent magnet | 22 | |
| po | Pole pairs of outer permanent magnet | 23 | |
| R1 | Inner radius of outer yoke iron | 96(mm) | |
| R2 | Outer radius of ring plate permanent magnet ring | 100(mm) | |
| R3 | Inner radius of the ring plate permanent magnet ring | 94(mm) | |
| R4 | Outer radius of low-speed permanent magnet ring | 90(mm) | |
| R5 | Inner radius of low-speed permanent magnet ring | 84(mm) | |
| R6 | Outer radius of inner yoke iron | 88(mm) | |
| hi | Inner yoke iron thickness | 15(mm) | |
| ho | Outer yoke iron thickness | 15(mm) | |
| e | Eccentricity | 3(mm) | |
| M | Magnetization | -890000(A/m) | |
| μ0 | Vacuum permeability | 4π×10-7 | |
| μ | Relative permeability | 1.0997 | |
| Br | Permanent magnet remanence | 1.21(M) | |
According to the operation principle of planetary gear with small tooth difference, the simplified structure of TRMG and equivalent model are shown in Figure 3.
By adding a speed around the axis of low-speed permanent magnet ring (contrary to the revolution speed of ring plate permanent magnet ring) to the whole mechanism, it can be converted into a conversion structure in which both ring plate permanent magnet ring and low-speed permanent magnet ring rotate on a fixed axis around their own axis, as shown in Figure 3 (b). The transmission ratio of the conversion structure is:
|
(13) |
Where, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): i_1
is equivalent model transmission ratio.
According to the equivalent model transmission ratio, the input speed of ring plate permanent magnet ring is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle n_\mbox{i}\mbox{=}70\mbox{r/}min}
, and the load torque of low-speed permanent magnet ring is Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle 124\mbox{N}\cdot \mbox{m}}
. The dynamic characteristic curve of equivalent model is shown in Figure 4.
From Figure 4, the electromagnetic torque and output speed of low-speed permanent magnet ring change regularly with time, finally converging to Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle 67\mbox{r/}min}
, around Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle 124\mbox{N}\cdot \mbox{m}}
, and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle M_{max}=130\mbox{N}\cdot \mbox{m}}
, meeting the design requirements. The ratio of input to output of speed and torque is about 22/23, which meets the transmission ratio design requirements in Equation (13).
5.2 TRMG start-up characteristic analysis
Changing the starting angle between ring plate permanent magnet ring and low-speed permanent magnet ring Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \beta }
. In Figure 2, point P, Q, U and V as starting point which are the left of interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[0,{\beta }_1\right]}
、 Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_1,{\beta }_2\right]}
、 Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_2,{\beta }_3\right]}
and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_3,{\beta }_4\right]}
.
Figure 5 shows the speed and torque characteristic curve with starting point P.
From Figure 5, it can be seen that from moment 0, the electromagnetic torque of low-speed permanent magnet ring gradually increases from 0 and changes periodically. Its rotating speed accelerates in opposite direction. So TRMG fails to start normally at point P. Because when Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [0,{\beta }_1]}
, the forward electromagnetic torque of low-speed permanent magnet ring is smaller than load torque, and the low-speed permanent magnet ring accelerates to rotate in opposite direction. When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_1,{\beta }_3]}
, the forward impulse on the low-speed permanent magnet ring cannot offset the reverse impulse generated in interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[0,{\beta }_1\right]}
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle (\Delta \mbox{PSQ}>\Delta \mbox{QUV)}}
, which prevents it from accelerating to the synchronous speed of rotating magnetic field. When Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_3,{\beta }_4]}
, the reverse acceleration continues under the combined action of reverse electromagnetic torque and the load torque, which eventually leads to start-up failure.
Figure 6 shows the speed and torque characteristic curve with starting point Q.
From Figure 6, it can be seen that from moment 0, the low-speed permanent magnet ring gradually increases and periodically changes from electromagnetic torque equal to load torque, and the speed gradually increases from 0 and stabilizes gradually after vibration. TRMG starts smoothly. This is because: when Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_1,{\beta }_3]}
, the forward electromagnetic torque impulse of the low-speed permanent magnet ring is greater than the load torque from moment 0, and the deceleration area Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
is avoided. So that the speed of the low-speed permanent magnet ring reaches synchronous speed of rotating magnetic field smoothly, and the speed and torque curve gradually converge.
Figure 7 shows the speed and torque characteristic curve with starting point U.
From Figure 7, it can be seen that from moment 0, the electromagnetic torque of the low-speed permanent magnet ring which is equal to the maximum torque, starts to decrease gradually and shows periodic changes. The speed first rotates forward and then decreases in reverse direction. This is because: when Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_2,{\beta }_3]}
, the forward torque impulse of the low-speed permanent magnet ring is larger than the load torque and causing it rotates forward. But its forward impulse is not sufficient to reach the synchronous speed of rotating magnetic field. After Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha }
increasing entry interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_3,{\beta }_4\right]}
, the low-speed permanent magnet ring continues to reverse accelerate rotation, eventually leading to TRMG start-up failure.
Figure 8 shows the speed and torque characteristic curve with starting point V.
From Figure 8, it can be seen that from moment 0, the electromagnetic torque of low-speed permanent magnet ring shows periodic changes and starts to decrease gradually from equal to the load torque. The speed accelerates reversely from 0. This is because: when Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \alpha \in [{\beta }_3,{\beta }_4]}
, the electromagnetic torque of the low-speed permanent magnet ring is less than the load torque, and the torque difference gradually increases with α increasing, which makes the low-speed permanent magnet ring reverse speed up rotation. After TRMG enters negative electromagnetic torque period, TRMG accelerates reverse rotates under the action of load torque and negative electromagnetic torque, which eventually leads to start-up failure.
6. Conclusions
(1) Based on structure mechanism of mechanical ring-plate drive mechanism, TRMG magnetic structure is proposed, and the operation mechanism and equivalent model of the model are elaborated. The dynamic verification model by finite element software shows that the simulation results are equivalent to the theoretical design output, which proves the established model is correct.
(2) Through the analysis of the starting position, it can be seen that Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \left[{\beta }_1,{\beta }_2\right]}
interval in Figure2 is the optimal starting interval of TRMG, and point Q is the optimal starting point.
(3) If TRMG can be started successfully, the deceleration interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{PSQ}}
of low-speed permanent magnet ring should be minimized. and increase acceleration interval Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://mathoid.scipedia.com/localhost/v1/":): {\textstyle \Delta \mbox{QUV}}
to achieve synchronous speed of coupled magnetic field.
Acknowledgement
This work was funded by the National Natural Science Foundation of China (Grant No.51375063), and also sponsored by the Natural Science Research Project of Liaoning Province Education Department (Grant No.JDL2020001) and partly funded by the Technological Innovation Research Foundation Project of Dalian (Grant No.2018J12SN071).
References
[1] Chen X.F., LI J.M., Cheng H., Li B., He Z.J. Research and Application of Condition Monitoring and Fault Diagnosis Technology in Wind Turbines. Journal of Mechanical Engineering, 47(9):45-52,2011.
[2] Kang Y.F., Luan J.Y., Tian Y., Zheng H.Q. Cao J.H., Application of the Order Tracking Analysis in Gear Wearing. Journal of Vibration and Shock. 25(4):112-113+118+180,2006.
[3] Jing L.B., Zhang Y., Huang Z., Chen J.L. Development Course and Research Question of Magnetic Gear. Journal of Mechanical Transmission. 43(1):165-170,2019.
[4] Atallah K., Rens J., Mezani S. Howe D., A novel “pseudo” direct-drive brushless permanent magnet machine. IEEE Transactions on Magnetics. 44(11): 4349-4352, 2008.
[5] Rens J., Atallah K., Calverley S.D., Howe D. A novel magnetic harmonic gear. IEEE Transactions on Industry Applications, 46(1): 206-212,2010.
[6] Jorgensen F., Andersen T., Rasmussen P. The Cycloid Permanent Magnetic Gear. IEEE Transactions on Industry Applications. 6(44): 1659-1665,2008.
[7] Rens J., Atallah K., Calverley S.D., Howe D. A novel magnetic harmonic gear. IEEE Transactions on Industry Applications. 46(1): 206-212,2009.
[8] Davey K., Hutson T., Mcdonald L., Hutson G. The design and construction of cycloidal magnetic gears. Electric Machines & Drives Conference, 2017.
[9] Huang H., Qu R., Bird J. Performance of Halbach Cycloidal Magnetic Gears with Respect to Torque Density and Gear Ratio. 2019 IEEE International Electric Machines & Drives Conference (IEMDC). 2019: 1977-1984.
[10] Hao W.N., Zhou J. The Cycloid Magnetic Gear Based on Halbach Array. Journal of Mechanical Strength. 39(1):226-229,2017.
[11] Wu S.Z., He W.D., Zhang Y.H. Analysis of Force and Contact Characteristics of Rotating Arm Bearings for RV Transmissions Mechanism. Journal of South China University of Technology (Natural Science Edition). 48(6):25-33,2020.
[12] Zhao D.L., Dang W.J., Sun W.P., Guo P.C. Influence of unbalanced magnetic pull on rub-impact rotor-bearing system. Journal of Huazhong University of Science and Technology(Natural Science Edition). 47(10):34-39,2019.
[13] Jian L., Chau K.T. Analytical calculation of magnetic field distribution in coaxial magnetic gears. Progress In Electromagnetics Research. 92: 1-16,2009.
[14] Lubin T., Mezani S., Rezzoug A. Analytical computation of the magnetic field distribution in a magnetic gear. IEEE Transactions on magnetics. 46(7): 2611-2621,2010.
[15] Deng Z., Nas I., Dapino M.J. Torque Analysis in Coaxial Magnetic Gears Considering Nonlinear Magnetic Properties and Spatial Harmonics. IEEE Transactions on Magnetics. PP(2): 1-11,2019.
Document information
Published on 21/10/21
Accepted on 08/10/21
Submitted on 02/08/21
Volume 37, Issue 4, 2021
DOI: 10.23967/j.rimni.2021.10.001
Licence: CC BY-NC-SA license
Share this document
Keywords
claim authorship
Are you one of the authors of this document?