3.2.2. Saw Cylinder Linear Velocity
The separation efficiency between seed cotton and boll husks is fundamentally determined by the linear velocity of the U-shaped saw cylinder. A force analysis of the boll husks provides a theoretical basis for determining the optimal rotational speed of the cylinder. The separation process can be categorized into two distinct scenarios: (1) scenarios without collision between boll husks and cleaning bars, and (2) scenarios with collision.
In non-collision scenarios, boll husks are subjected to four mechanical loads during U-shaped saw cylinder operation: centrifugal force generated by rotational motion, fiber tensile force, aerodynamic drag, and gravitational force. The volume of the boll husks is relatively small, and the centrifugal force, which dominates at 25–35 times the boll husks’ self-weight [
16], renders both aerodynamic drag and gravitational force negligible. The force distribution is shown in
Figure 5a. To achieve the separation of seed cotton and boll husks, the following conditions must be satisfied:
where
F1 is the centrifugal force generated by the rotational motion, N;
T1 is the fiber tensile force, N;
m1 is the boll husks’ weight, kg;
v is the saw cylinder’s linear velocity, m/s; and
r1 is the saw cylinder’s radius, m.
The experimental measurements indicated an average detachment force of 0.35 N between seed cotton and boll husks. Based on calculations from Equations (1) and (2), if centrifugal force alone is used to remove the boll husks, the linear velocity of the U-shaped saw cylinder must be at least 21.7 m/s. However, excessive rotational speed causes two critical issues: (1) seed cotton not firmly gripped by the sawteeth detaches, increasing fiber loss; and (2) accelerated wear on the U-shaped saw cylinder shaft and bearings reduces their service life. To solve these problems, a series of cleaning bars are arranged around the U-shaped saw cylinder. By means of collision with these bars, the separation efficiency between seed cotton and boll husks is enhanced, as shown in
Figure 5b.
To achieve effective cotton–impurity separation, the following critical conditions must be satisfied:
where
I1 is the collision force between the boll husks and cleaning bars, N; Δ
v is the velocity variation amplitude of the boll husks, m/s; and Δ
t is the collision duration, s.
The linear velocity of the U-shaped saw cylinder can be reduced to 5–10 m/s following the circumferential integration of cleaning bars [
17].
3.2.3. Sawtooth Design
The sawteeth are classified into two types: straight and arc-shaped.
Figure 6 illustrates the structural schematic of the straight sawteeth. The working angle (
α) directly influences the cotton-grabbing capacity: a larger
α enhances the gripping force but may affect the brushing effect. The tip angle (
φ) governs sawtooth strength, with higher
φ values improving durability; empirical data from prior studies established
φ as 27°. Tooth spacing (
l) exhibits a trade-off because increasing
l increases the fiber load capacity while reducing the holding force. Similarly, tip depth (
h) must be matched to the cotton fiber thickness to balance load capacity and structural integrity [
18,
19,
20].
To determine the specific structural parameters of the sawteeth, a force analysis must be conducted on the seed cotton during motion. During sawtooth-driven rotation, the seed cotton is subjected to four principal forces: a centrifugal force induced by high-speed rotation, a surface friction force from serration contact, an aerodynamic drag force, and a gravitational force. Since the centrifugal force during operation is 25–35 times the seed cotton’s weight, the gravitational force can be neglected. The force distribution acting on the seed cotton is shown in
Figure 7. To prevent the premature detachment of the seed cotton, the following conditions must be satisfied:
Including:
where
F2 is the centrifugal force acting on seed cotton, N;
Fk is the aerodynamic drag force,
N;
f is the frictional force;
m2 is the weight of seed cotton,
m2 = 0.24 g;
C is the drag coefficient,
C = 0.44 [
21];
ρ is the air density,
ρ = 1.205 kg/m
3;
S is the windward area of seed cotton,
S = 1.45 × 10
−3 m
2;
μ is the friction coefficient,
μ = 0.34; and
α is the sawtooth working angle, (°).
Based on Equation (5) and in conjunction with the force analysis of seed cotton motion, the following is derived:
Substituting Equation (6) into Equation (7) yields Equation (8).
Let
, simplify Equation (8), and determine the mathematical expression for the working angle
α:
After calculation and rounding, the working angle α is determined to be 42°.
In the
ABC triangle of
Figure 6, the mathematical expression for the sawtooth pitch
l is determined by combining the area formula of a triangle with the laws of sines and cosines:
where
h is the tooth tip depth, designed to match the cotton layer thickness with
h = 5.7 mm;
φ denotes the tooth tip angle, which is designed to meet strength requirements and is preliminarily set to 27°; and the calculated sawtooth pitch
l is 9.8 mm.
In summary, the specific structural parameters of the sawteeth are listed in
Table 3.
In
Figure 6,
lbc denotes the contact length between the straight sawteeth and the fibers. The longer
lbc is, the greater the number of fibers in contact with the sawteeth. This increase leads to stronger friction forces between the fibers and the sawteeth, thereby making the cotton less prone to premature detachment. In the
ABC triangle
, the mathematical expression for
lbc is derived as follows:
where
lbc is the contact length between the straight sawteeth and the fibers, mm, and
δ is the angle between the relative velocity of seed cotton and the linear velocity of the sawteeth. Theoretically, the sum of
α,
φ, and
δ equals 90°; however, due to the fillet at the tooth root,
δ is set to 16°.
The schematic diagram of the arc-shaped sawtooth structure is shown in
Figure 8. Based on the arc length formula, the contact length
between the arc-shaped sawteeth and the fibers is determined as follows:
where
is the contact length between the arc-sawteeth and the fibers, mm;
R is the arc radius, which is designed to be 10 mm in this study; and
θ is the central angle of the arc, (°).
In the
ABD triangle, the following relationship is derived using the law of sines:
where
lbd is the distance between b and d, and
ε is the newly introduced working angle, °.
In the
OBD triangle, the following relationship is derived using the law of cosines:
Therefore, the mathematical expression for the contact length
of the arc-shaped sawteeth is:
Compared to straight sawteeth, an arc-shaped sawtooth introduces an additional contact length
l′:
Figure 9 illustrates the relationship between the newly introduced working angle
ε and the additional contact length
l′ of the arc-shaped sawteeth under the following conditions: working angle
α = 42°; arc radius
R = 10 mm; teeth pitch
l = 9.8 mm; and
δ = 16°. The curve demonstrates that
l′ increases with
ε. However, due to constraints imposed by the teeth geometry and strength limitations,
ε cannot be infinitely increased. In this study,
ε is determined to be 16°, resulting in
l′ = 5.19 mm. The structural parameters of the arc-shaped sawteeth are listed in
Table 4.