“三角洲” 是一种机器人或打印机,其头部运动是依靠呈三角摆放的三对并联臂。一对平行的并联臂保持头部的水平,并联臂的运动使头部在三个维度上自由移动。三角洲有很多的方案,有些是可以简单制作使用的。
并联臂有两种常见方案:
还有另一种没有刚性框架的方案是将头部悬挂在绳子上用绳子驱动。 有几个例子是 Skydelta 和 suspended delta的。
线性三角洲的运算很简单,因为滑块沿直线运动的,所以头部的水平运动与机架的垂直运动通过勾股定理(对角线长度的平方等于三角形边的平方和,三角形有人必须是直角三角形)。 这里对角线是臂长,常数,垂直分支是平台和托架的相对垂直位置,水平分支是平台和托架的相对水平位置。
数学不难,但对于3D打印机来说必须做很多平方根。 基于8位处理器的主板很辛苦的计算,对这些用8位处理器的三角洲进行了很多软件优化。 32位主板正在成为三角洲打印机更常见的主板选择,因为它们具有更快的处理器。 在不对称设计进行了测试,三个滑块可以在非等边三角形上,尤其是角度为 90° 和 180° 的“方形”三角洲。

以效应器为中心的臂角是并联臂长度、最小角度和并联臂在最大直径时的角度的结果。 对于 20° 的最小角度,对于最大直径的臂垂直线,该角度约为 60°,但如果增加最小角度,它可能会更高。 22° 的最小角度将与垂直臂产生 63° 的角度。
由于间隙问题,尤其是冷却风扇或效应器附件,并联臂可能无法达到垂直角度。 在这种情况下,对于给定的最小角度,臂长可能会减少,而效应器处于中心时的角度会更低。
另一方面,一些打印机的手臂能够垂直越过(例如 Rostock Max)。


当效应器处于最大直径时,最小臂角是基本设计参数之一。 它对效应器的稳定性、精度和滑架速度很重要。 对于给定的效应器水平速度,低角度会导致高滑架速度。 低角度也会降低效应器的稳定性。 一般来说,20°角被认为是一个实际的最小值,并导致滑架速度比效应器水平速度高2.75倍。 一些理论上最小角度为 15° 的打印机可能会在其最大直径处出现失步。

壁杆角度的加速系数
| 角度 | 速度倍数 |
| 22.5° | 2.41 |
| 20° | 2.75 |
| 17.5° | 3.17 |
| 15° | 3.73 |
| 12.5° | 4.51 |

手臂空间不影响运动计算,但对效应器稳定性很重要。 最小偏移获得最佳稳定性,该偏移具有最大可能的臂空间(最小化 b 尺寸)。

对于给定的最小角度,可到达区域是一个带有凸出边的三角形,三角形的末端朝向柱子,在不影响柱子的情况下无法进入。 然后,为简单起见,可到达区域通常被认为是圆形的。 当一个人想在打印区域中刻一个矩形或正方形时,评估真正的可到达区域可能会很有趣。 配件(皮带和风扇)对于实际可用区域至关重要。
示意图

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This is the fact that an effector resist to tilting moments. The tilt may displace the hotend nozzle and creates imprecision. It also have an effect on level measurement sensor while the sensors are offset from the hotend. Two things have important effect on an effector stability:
The moment which will induce tilt will be created by :
What is also very important is the position of the hotend to minimize the effect of effector tilt. Experience show that a nozzle near the effector plane seems the best solution. However, care shall be taken to limit the raise of the center of gravity, to avoid creating dynamic moments.
Understanding that there are other causes that the effector stability to nozzle movement imprecision, it is however interesting to quantify the displacement due to geometrical instability.
A coefficient could be defined, that we may called TES, for tilt effector stability, which will not quantify the effector instability, but its effect on the hotend, by combining the moment effect and the displacement related to the distance between the virtual articulation and the nozzle location.
a being the lever due to arm space (see drawing) b being the space between balls (articulations)
TES = (Arm space)²/b, Dimension units shall be mm.
It is important to note that the TES does not depend from arm length, only effector geometry. Indeed, the arm stiffness in their axis is huge compared to other elements, notably articulation stiffness, so the arm length have nearly no effect on tilting stability. This is why you could install the small Kossel mini effectors on large printers without problems. It shall be noted that for merged articulations, this coefficient will be infinite.
This coefficient is calculated in the OpenScad delta simulator.
The practical improvements added by a good geometry is closely related to the quality of the mechanical implementation. By example, if you widen the arm space to improve stability, but the side extensions on the carriage to reach the new width add excessive flexibility, you may have at the end reduced the real stability. It shall be noted that wider arm space does not raise or decrease the moment and only help to fight play in articulation. If your problem is the rotation of the carriage, that is the carriage which shall be reinforced, no geometry can help.


已经失效! Thinkyhead Deltabot calculator 三角洲计算器,输入数字进行模拟。

Rotational delta are a quite common research topic, notably for university students.
Some people have done Delta simulation on CAD/Math software, but not publicly release them.