The following paragraphs serve for the specification of the geometrical values, which are needed in the input masks.
Fields with a grey background cannot be edited because they are either dependent on other variables and are therefore determined by REX/PSI (e.g. the channel width) or are defined by the input in previous screw zones (e.g. the diameter).
Some values, such as the length $L$ or the pitch $t$, can be specified either as absolute values or as dimensionless values in relation to the diameter $D$.
As the leakage is taken into account in the calculations, the following definitions must be observed:
The only exceptions here are the cylindrical and the conical shearing sections. For these two shear sections, the shear gap height from the base of the shear section to the cylinder surface must be entered.
In the individual screw zones, radii can be specified on the driving ($r_1$) and non-driving ($r_2$) flank of the screw channel as well as a flank angle of the non-driving flank. The driving flank, also known as the active flank, represents the side of the screw flight that pushes the plastic towards the screw tip due to the screw rotation. The non-driving flank, also known as the passive flank, is therefore the other side of the screw flight.
The following figure shows three examples for entering the radii and the flank angle.
Basically, the width of the channel results in
$$b=\frac{t \cdot cos(\varphi) - i \cdot e}{i}$$
$$\text{with}$$
$$tan(\varphi)=\frac{t}{\pi \cdot \overline{D}}$$
$$\text{and}$$
$$\overline{D} = D-h$$
with the pitch $t$, the pitch angle $\varphi$, the flight width $e$, the nominal screw diameter $D$, the channel depth $h$ ,the number of channels $i$ and the effective diameter $\overline{D}$.
In the figure above, however, areas that reduce the channel cross-section are marked in red. As REX/PSI always calculates with a simplified rectangular channel, the reduction of the channel cross-section is taken into account by a reduced channel width:
$$b_{effective}=\frac{b \cdot h-A_{radii,\gamma}}{h}$$
Dividing the actual channel cross-section by the channel height $h$ results in the effective channel width.
The channel cross-section $A_{radii,\gamma}$ is calculated as follows: $$A_{r<h,\gamma=90°} = \frac{r^2}{4} (4 - \pi)$$
$$ A_{r<h,\gamma>90°} = r^2 \left( \frac{1 + \cos \gamma}{\sin \gamma} - \pi \frac{180^\circ - \gamma}{360^\circ} \right) - \frac{1}{2} \frac{h^2}{\tan \gamma} $$
$$ A_{r>h,\gamma=90°} = \frac{1}{2}(r + h) r \sin \left[ \arccos\left(1 - \frac{h}{r}\right) \right] - \frac{\pi r^2}{360^\circ} \arccos\left(1 - \frac{h}{r}\right) $$
The calculation of the channel cross-section takes into account the actual channel width $b$, the effective channel width $b_{effective}$, the channel height $h$, the flight width $e$ and the screw clearance $\delta$. The channel volume is made up of 2 areas:
$$A_{total}=A_{channel}+A_\delta$$ $$\text{with}$$ $$A_{channel} = b_{effective} \cdot h$$ $$\text{and}$$ $$A_\delta = \delta \cdot (b+e)$$
The channel volume is calculated by multiplying the channel cross-section by the unwound channel length $L_{channel}$:
$$V_{channel} = A_{total} \cdot L_{channel}$$ $$\text{with}$$ $$L_{channel} = \frac{L_{zone}}{sin(\varphi)}$$
with the pitch angle $\varphi$