Jco - 2011!12!657 Locking The Screw After Rapid Palatal Expansion
Jco - 2011!12!657 Locking The Screw After Rapid Palatal Expansion
Jco - 2011!12!657 Locking The Screw After Rapid Palatal Expansion
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Dr. Franchi
Dr. Baccetti
Dr. Huanca Ghislanzoni is a doctoral student, Department of Human Morphology, University of Milan, and Dr. Franchi is an Assistant Professor,
Department of Orthodontics, University of Florence, Florence, Italy, and a Thomas M. Graber Visiting Scholar, Department of Orthodontics and
Pediatric Dentistry, School of Dentistry, University of Michigan, Ann Arbor; e-mail: lorenzo.franchi@unifi.it. Dr. Baccetti, who was killed in a tragic
accident in November (see The Editors Corner, JCO, November 2011), was a Contributing Editor of the Journal of Clinical Orthodontics, an Assistant
Professor, Department of Orthodontics, University of Florence, and a Thomas M. Graber Visiting Scholar, Department of Orthodontics and Pediatric
Dentistry, School of Dentistry, University of Michigan.
657
658
JCO/DECEMBER 2011
Ff
F//
0.4mm
1.5mm
Fig. 3 Screw characteristics and resulting forces. A. Screw pitch and thread slope. B. Direction of forces.
pitch
= arctan diameter
(Eq. 1)
By applying this equation to the A0620
screw, the thread-slope angle, , is shown to be
4.9.
The forces from the stretched maxillary tis
sues, acting parallel to the long axis of the screw,
may be broken down into two parts (Fig. 3B): F//
(parallel to the threads) and F (perpendicular to
the threads). F// alone could theoretically cause the
screw to turn back because it acts as a tangential
force, creating a moment around the long axis of
the screw. F is assumed to be the force responsible
for frictional resistance to turning.
The force of static friction is calculated by
multiplying the normal force by the coefficient of
friction, which for stainless steel is about .74.18
659
660
JCO/DECEMBER 2011