Delta-3 (also spelled $\delta_3$) is a simple yet difficult to visualise concept.
I suppose that the best way to understand it is by comparing a rotor with a built-in delta-3 with one without it. The following two rotor heads are both taken from Wikipedia (plus a couple of colorful lines from my side): the first one is the main rotor head of a Bell 222, the second one is the tail rotor of a Robinson R44.
Main rotor of Bell 222. Source: Wikimedia Commons
Tail rotor of Robinson R44. Source: Wikimedia Commons
For the Bell 222, the red line of the pitch hinge is perpendicular to the blue line of the flapping hinge (also called teetering hinge in this particular design). For the R44, the red line and the blue one are not perpendicular but intersect at some 45°. Hopefully this difference is visibile despite the different perspective of the pictures. This not-perpendicular intersection like in the R44 is the delta-3 angle.
Now, when a blade of the B222 flaps upward... well it just flaps upward. When the blade of the R44 flaps upward (actually "outward" is maybe a more correct term for a tail rotor but for ease of comparison I stick with upward) it flaps upwards... and it reduces it's pitch, exactly because these two axis are not perpendicular due to delta-3.
That's not very easy to represent but it could become clearer looking at an extreme case: starting with the B222 configuration and its 90° shifted blue and red line, let's reduce this angle (i.e. increase delta-3); we get to the R44 configuration with its 45° between blue and red line; now let's reduce this angle again (i.e. further increase delta-3) till we get to the extreme case where blue and red line overlap (i.e. delta-3=90°): now flap and pitch have become the same thing, they both lie on the same axis, they are coincident, 1° of flap coincides to 1° of pitch. To sum up:
- blue and red lines perpendicular (B222) $\Leftrightarrow$ $\delta_3=0°$ $\Rightarrow$ flap and pitch fully decoupled
- blue and red lines coincident $\Leftrightarrow$ $\delta_3=90°$ $\Rightarrow$ flap and pitch fully one-to-one coupled
- $\delta_3$ between 0 and 90° (R44) $\Rightarrow$ flap and pitch partially coupled.
(This latter partial coupling is mathematically translated as $\theta_{\delta_3}=\beta tan \delta_3$, where $\theta_{\delta_3}$ is the change in pitch due to the flapping $\beta$. Maybe if you have some Lego technic laying around you could try it out and verify it live).
What's the benefits of that? As said, when the blade flaps upward (outward) the delta-3 makes its pitch reduces which, in turn, reduces the aerodynamic thrust generated by the blade which, in turn, reduces its flapping. The opposite is true when the blade flaps downward (inward) i.e. the delta-3 makes the pitch increases, increasing its thrust and therefore its flapping:
- blade flaps $\Rightarrow$ due to $\delta_3$ pitch reduces $\Rightarrow$ lift reduces $\Rightarrow$ flap reduces
So delta-3 is a simple cinematism used to limit the amount of flapping of the blades of the rotor.
This has a twofold outcome:
- clearance between tail rotor and tailboom is reduced giving a shorter and lighter shaft;
- flapping produces also lead-leg movement via the Coriolis force; if flap is reduced also lead-leg movement is reduced and it can be reduced to the point that the lead-leg hinge can be disposed of, as in the R44.
Free weight saving is always good in the aerospace world.
Bonus material
Delta-3 is used exactly for the same reason also on the main rotor, anyway in a milder way since flapping is the physical effect which permits the control of the helicopter, so a compromise between shorter/lighter mast and controllability is needed here.
Since on the red line only 2 blades can lie, for rotors with 3 or more blades the delta-3 effect is obtained with a different cinematism: if someone is interested in it, I could expand this answer.