2016
DOI: 10.1177/0040517516641363
|View full text |Cite
|
Sign up to set email alerts
|

Mathematical modeling, simulation and validation of the dynamic yarn path in a superconducting magnet bearing (SMB) ring spinning system

Abstract: The new concept of a superconducting magnetic bearing (SMB) system can be implemented as a twisting element instead of the existing one in a ring spinning machine, thus overcoming one of its main frictional limitations. In the SMB, a permanent magnet (PM) ring rotates freely above the superconducting ring due to the levitation forces. The revolution of the PM ring imparts twists similarly to the traveler in the existing twisting system. In this paper, the forces acting on the dynamic yarn path resulting from t… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

1
21
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 17 publications
(22 citation statements)
references
References 21 publications
1
21
0
Order By: Relevance
“…The second boundary condition at the guide eye of the PM ring can be defined from the equation of motion 14 where T1 is the yarn tension at the bottom of the balloon (into the PM ring contact), ÎŒ 1 is the friction coefficient between the yarn and the yarn guide eye on the PM ring, and α is the wrapping angle of the yarn on the PM ring guide eye section. As shown in Figure 2, ϕ is the angle between the tangential and the radial at the beginning of the yarn winding, normalsinâĄÏ•=ba; |normal normalâ€Č≡normald()normalds; where b is the radius of the wind-point on the bobbin and dR is the rotational damping coefficient of the PM ring 15 where CdR is a proportional constant and Re is the Reynolds number.…”
Section: Semi-analytical Solutionmentioning
confidence: 99%
“…The second boundary condition at the guide eye of the PM ring can be defined from the equation of motion 14 where T1 is the yarn tension at the bottom of the balloon (into the PM ring contact), ÎŒ 1 is the friction coefficient between the yarn and the yarn guide eye on the PM ring, and α is the wrapping angle of the yarn on the PM ring guide eye section. As shown in Figure 2, ϕ is the angle between the tangential and the radial at the beginning of the yarn winding, normalsinâĄÏ•=ba; |normal normalâ€Č≡normald()normalds; where b is the radius of the wind-point on the bobbin and dR is the rotational damping coefficient of the PM ring 15 where CdR is a proportional constant and Re is the Reynolds number.…”
Section: Semi-analytical Solutionmentioning
confidence: 99%
“…[5][6][7] Superconducting magnetic bearing (SMB) systems have been investigated to provide a contact-free method of yarn winding and twisting to replace the original ring/traveler system in ring spinning machines. [8][9][10][11] While this is a novel method for eliminating frictional heat of the ring/traveler system, it cannot be immediately applied for the reasons of installation and cost. Vibration has also been added to the ring/traveler system, to decrease the contact frequency between traveler and ring, thereby reducing the frictional heat.…”
mentioning
confidence: 99%
“…Among researches related to textile systems, there are quite a few that focus on the movement and dynamics of textile flexible bodies, such as yarns, filaments, or fabrics. For example, Hossain et al [8][9][10] carried out mathematical modeling research on the yarn movement state in the ring-spinning system. A similar study is Tang et al, 11 which adds a part of the experimental verification.…”
mentioning
confidence: 99%
“…For example, Hossain et al. 8–10 carried out mathematical modeling research on the yarn movement state in the ring-spinning system. A similar study is Tang et al., 11 which adds a part of the experimental verification.…”
mentioning
confidence: 99%