@TorontoBuilder would your hood fan approach also work for open frame printers?
Of course this design will work with both open frame and enclosed printers... with certain caveats. This advice also applies ONLY to 3D printing risks. I'll address other risks and improvements after this section.
Several factors impact exhaust air capture, the airflow volume, airflow speed, and particle mass. Typically, higher mass requires higher velocity to move it. Because 3D printing particulates and VOCs are microscopic, our main concern is generating enough airflow speed to overcome background air movement in the room.
Our available air volumes are limited by standard residential exhaust fans, while our capture velocities depend on the open area between the hood and the work surface.
For the model shown the hood area is 40" x 20", which is 800 square inches, or 5.6 square feet in area. The average height above the work surface is 2 feet 8 inches for a total exhaust envelope of about 15 cubic feet in volume.
The ECM motor bath fan I plan to use has 3 speeds options and the ecm motor assures (within reason) that the full airflow is delivered with differing exhaust duct configurations.
On the low setting of 50 CFM the volume of air under the hood is turned over 3.33 times per minute. Looking at it another way the a air is completely replaced once every 18 seconds.
On the medium setting of 80 CFM the volume changes 5.33 times per minute, or is completely replaced once every 11.2 seconds.
On the high setting of 100 CFM the volume changes 6.67 times per minute, or is completely replaced once every 9 seconds.
Even at the lowest setting that is a very high ventilation rate enough to prevent fumes escaping the capture envelope below the exhaust hood.
BUT..
When an open canopy hood hangs
above a source without side walls, air rushes in from all four open sides between the table and the hood rim. The volume of air exhausted is spread over this wide perimeter area, so the velocity is low.
In local exhaust ventilation design, the standard equation used to calculate the required airflow rate for a free hanging canopy hood is Q = 1.4 x P x D x V. This formula determines the volumetric airflow needed to capture rising contaminants across the open gap between the source and the overhead canopy.
Rearranged to solve for capture velocity v = cfm / (1.4 x P x D) where:
P = perimeter in feet which is the distance around all open edges of the hood.
D is the distance from the workbench to the bottom rim of the hood.
1.4 is a correction factor that accounts for uneven air distribution around the perimeter corners.
Therefore,
v = 50 / 1.4 x 10' x 2.68'
v = 50 / 37.52
v = 1.33 fpm
Not that high a velocity at all.
But the velocity increases as soon as the air passes the bottom plane of the hood opening, because the area decreases from an effective area of 37.52 sq. ft. (26.8 sq. ft. x 1.4 correction factor) to 5.6 square feet. At the bottom plane as air enters the hood the velocity calculation is simplified to a face velocitycalculation. V = cfm / area in square feet which in our case yields v = 50 / 5.6 = 8.9 fpm.
This still works for 3D printing because of thermal buoyancy. The heated print bed and hot end create a rising column of warm air. You don't need high suction at the table because heat naturally carries the particulates and VOCs upward into the hood's capture zone.
We aid this draft effect by lowering the hood so that the top of the printer breaks the bottom plane of the hood... and sit inside the hood space.
Once that warm plume crosses the bottom rim of the hood, the tapered walls squeeze the airflow from 5.6 square feet down to 1 square foot accelerating the air velocity from ~9 FPM at the plane up to 50 FPM at the fan opening so nothing stalls or spills back out.
Where the design hits its limits is with cold fumes and room temperature vapours, such as resin VOCs, isopropyl alcohol, adhesives, or solvent paints which lack that thermal lift. Without heat to carry them up the 32 inch gap, a cross draft can push them sideways before they ever reach the hood.
Even with a warm FDM printer, placing the setup near an HVAC supply register, open window, or busy walkway can shear the warm plume off center before it enters the hood. The same could apply if the printer uses high power parts cooling fans that blow air out of the capture envelope.
To make this hood handle room drafts, or open printers with high speed parts cooling fans, or non heated tasks, you have to shrink that open perimeter, either by lowering the hood closer to the source or by adding side and rear drop panels to block cross breezes and force all incoming air through a smaller front opening.
Closing off three sides converts the open canopy into a three sided booth, changing the formula to standard face velocity:
v = cfm / area
Instead of pulling air weakly from all four sides, the fan now draws air strictly through the single open front window. The sides and back block external air movement from affecting thee exhaust of contaminants, and keep parts cooling fans from pushing fumes out of the containment envelope.
v = 50 / ((40" x 32") / 144) = 50 / (1280 / 144) = 50 cfm / 8.88 sq ft = 5.63FPM
5.63 FPM across a full 32 inch high opening is fine for warm FDM printing with high speed part cooling fans, since the walls bounce the fan wash upward into the hood, but for cold fumes or heavy solvents, you should bump the fan to 100 CFM and add a partial front drop/sash, that will leave a shorter working window at the bottom. This would yield the following:
v = 100 / ((40" x 12") / 144) = 100 / (480 / 144) = 100 cfm / 3.33 sq ft = 30.03 FPM
Or since 40" is pretty wide an opening, you could use sliding door panels across the front, and access only a smaller area as needed. Say three panels 14" wide... making the widest possible opening about 14" which yields these calculation:
v = 50 / ((14" x 32") / 144) = 50 / (448 / 144) = 50 cfm / 3.11 sq ft = 16.07 FPM
v = 100 / ((14" x 32") / 144) = 100 / (448 / 144) = 100 cfm / 3.11 sq ft = 32.14 FPM