CM Dent J Vol. 42 No. 1 January-April 2021133
and stress were also transferred to the second
molar, causing posterior tooth movement and whole
arch distalization. Thus, this nite element nding
may be used as evidence to support the theory of en-
masse distalization, which proposes that the entire
maxillary dentition can be effectively moved after
applying force to an anteriorly located hook.
(24)
In this study, the results of stress distribution in
the PDL were examined in terms of the von Mises
stress. It was used to represent the overall stress
of a multi-axial stress just the same as it has been
applied in previous studies.
(22,24,35-37)
The stress on
the teeth close to the point of force application at the
retraction hook, was more concentrated than on some
other teeth in positions farther from the hook. With
0-mm- and 2-mm- hooks, the highest level of stress
was found at the cervical third of canine. With the
other lengths, the highest level of stress was found
on the apex of lateral incisor, which was also close
to the point of force application. These outcomes are
in agreement with those of Sung et al.
(24)
The results revealed that the length of retraction
hook highly relates to the types of tooth movement.
Changing the length of retraction hook affects the
distance between the line of action of force and the
CRes. When distalization force is applied to low-
level hooks, the line of action of the force passed
below the CRes and induced clockwise moment,
resulting in steepening of the occlusal plane. Conse-
quently, the anterior teeth had palatal crown tipping
and extrusion. The posterior teeth tipped distally
and substantially intruded (Figure 7A). The level of
stress was high at the distal root of the second molar
because the posterior teeth were intruded. More-
over, the constructed tuberosity distal to the second
molar and the boundary conditions at the back of the
model may have strongly resisted the distalization,
resulting in high stress in the distal root of the second
molar (Figure 4A & B). On the other hand, the line of
action of the force passed above the CRes and
generated counterclockwise moment, resulting in
upward rotation of the occlusal plane. The labial
aring of anterior teeth was observed, and the pos-
terior teeth were slightly extruded (Figure 7C). The
stress in the PDL of posterior teeth was less than
that with shorter hooks because extrusion occurred
(Figure 4D & E).
When a distalization force was applied to a
4-mm hook, the line of action of the force passed
near the CRes, rather than passing through it, and a
low moment was generated. The line of force may
have passed either slightly below or slightly above
the CRes; therefore, the low moment may have been
either clockwise or counterclockwise, respectively
(Figure 7B). All maxillary teeth moved distally along
the occlusal plane with minimal intrusion or tipping.
The location of the miniscrew at the Modied IZC
was higher than the CRes resulted in a distal and
upward direction of the line of action of force,
generating intrusion and distalization of the maxillary
dentition. In whole arch distalization, the entire
maxillary dentition did not undergo pure bodily
movement. The reason may be archwire deection
of the force system, causing a relatively some degree
of tipping movement.
All of the tooth displacement patterns studied
correspond with the results of previous studies that
used different lengths of retraction hook for whole
arch distalization with interradicular miniscrews
(24)
,
and for distalization of the posterior teeth with
modied IZC miniscrews.
(38)
The distalization force can be divided in to
three axes which affect to the occurred displacement
pattern. The amount of force in each axis was
calculated and represented as Fx, Fy, and Fz. Fx was
a lateral force along the x axis; Fy was an intrusive
force along the y axis; Fz was the horizontal force
or distalization force along the z axis. These forces
were calculated from the resultant force formula of
three vectors using the angle values in this nite