The Smell of Molten Projects in the Morning

Ed Nisley's Blog: Shop notes, electronics, firmware, machinery, 3D printing, laser cuttery, and curiosities. Contents: 100% human thinking, 0% AI slop.

Category: Electronics Workbench

Electrical & Electronic gadgets

  • FT82-43 Slit Toroid: Armor

    Given the fragility of ferrite toroids in general and slit toroids in particular, a touch of up-armoring seems sensible:

    FT82-43 toroid - mounted
    FT82-43 toroid – mounted

    The solid model includes a toroid shell with roughly the right curves:

    Toroid Mount - Show layout
    Toroid Mount – Show layout

    That puts a nice rounded shape on the bottom of the armor, not that that makes much difference:

    Toroid Mount - Build layout
    Toroid Mount – Build layout

    The central hole passes a 4-40 brass, nylon, or stainless steel screw. Most of the magnetic field stays within the ferrite and, heck, this isn’t a crazy-sensitive analog application, so even an ordinary steel screw shouldn’t cause any particular problems.

    The rectangular (not pie-wedge) slit barely passes the Hall effect sensor.

    I’ll pour some clear epoxy over the toroid, with tape masking the ferrite core and sealing the ends, to immobilize the windings. That sounds like a good idea after calibration and suchlike.

    The OpenSCAD source code, which should be sufficiently parametric that I can crank ’em out for all the other toroids large enough to accept a screw:

    // Toroid coil mounting bracket
    // Ed Nisley - KE4ZNU - August 2014
    
    Layout = "Mount";			// Coil Mount Build Show
    
    //- Extrusion parameters must match reality!
    //  Print with 4 shells and 3 solid layers
    
    ThreadThick = 0.20;
    ThreadWidth = 0.40;
    
    HoleWindage = 0.2;			// extra clearance
    
    Protrusion = 0.1;			// make holes end cleanly
    
    AlignPinOD = 1.70;			// assembly alignment pins: filament dia
    
    function IntegerMultiple(Size,Unit) = Unit * ceil(Size / Unit);
    
    //----------------------
    // Dimensions
    
    ID = 0;												// subscripts for cylindrical objects
    OD = 1;
    LEN = 2;
    
    Coil = [10.25,23.50,8.3];							// wound toroid core
    
    SensorThick = 2.0;
    
    BaseThick = IntegerMultiple(1.0,ThreadThick);		// baseplate under coil
    WallThick = IntegerMultiple(1.0,ThreadWidth);		// walls beside coil
    
    ScrewHoleDia = 4.0;									// allow alignment slop around 3 mm / #4 screws
    
    //----------------------
    // Useful routines
    
    module PolyCyl(Dia,Height,ForceSides=0) {			// based on nophead's polyholes
    
      Sides = (ForceSides != 0) ? ForceSides : (ceil(Dia) + 2);
    
      FixDia = Dia / cos(180/Sides);
    
      cylinder(r=(FixDia + HoleWindage)/2,
               h=Height,
               $fn=Sides);
    }
    
    module ShowPegGrid(Space = 10.0,Size = 1.0) {
    
      RangeX = floor(100 / Space);
      RangeY = floor(125 / Space);
    
    	for (x=[-RangeX:RangeX])
    	  for (y=[-RangeY:RangeY])
    		translate([x*Space,y*Space,Size/2])
    		  %cube(Size,center=true);
    
    }
    
    //----------------------
    // Basic coil shape
    
    module CoilShape() {
    	
    CornerRadius = min((Coil[LEN] / 2),((Coil[OD] - Coil[ID]) / 2))  / 3;
    MidRadius = (Coil[ID] + Coil[OD]) / 4;
    HalfX = (Coil[OD] - Coil[ID]) / 4 - CornerRadius;
    HalfY = (Coil[LEN] / 2) - CornerRadius;
    
    echo(CornerRadius,MidRadius,HalfX,HalfY);
    	
    	color("Goldenrod")
    	render(convexity = 2)
    		rotate(180/20)
    			rotate_extrude(convexity=3,$fn=20)
    				translate([MidRadius,0])
    					hull() 
    						for (i=[-1,1],j=[-1,1])
    							translate([i*HalfX,j*HalfY])
    								circle(r=CornerRadius,$fn=24);
    }
    
    //----------------------
    // Mount
    
    module Mount() {
    
    	difference() {
    		rotate(180/20)
    			cylinder(h=(BaseThick + Coil[LEN]),d=(Coil[OD] + 2*WallThick),$fn=20);
    		
    		translate([0,0,-Coil[LEN]])							// make screw hole
    			rotate(180/6)
    				PolyCyl(ScrewHoleDia,3*Coil[LEN],$fn=6);
    			
    		translate([0,0,BaseThick + Coil[LEN]/2])			// set bottom curve
    			CoilShape();
    			
    		translate([0,0,BaseThick + Coil[LEN]])				// clear out top
    			CoilShape();
    			
    		translate([(Coil[ID]/2 + Coil[OD]/2),0,0])
    			cube([Coil[OD],SensorThick,3*Coil[LEN]],center=true);
    	}
    }
    
    
    ShowPegGrid();
    
    if (Layout == "Coil") {
    	CoilShape();
    }
    
    if (Layout == "Mount")
    	Mount();
    
    if (Layout == "Show") {
    	Mount();
    	translate([0,0,(BaseThick + Coil[LEN]/2)])
    		CoilShape();
    }
    
    
    if (Layout == "Build") {
    	Mount();
    }
    
  • FT82-43 Slit Toroid: Construction

    The FT82-43 toroid slit easily enough, using the same diamond-wheel Sherline setup as for the smaller toroids:

    FT82-43 toroid - slit
    FT82-43 toroid – slit

    I’m pretty sure that chip at 1 o’clock happened while it was clamped in the vise between two cardboard sheets, but I haven’t a clue as how it got that much force. In any event, that shouldn’t affect the results very much, right up until it snaps in two.

    Although the current will come from a (rectified) 120 VAC source, the winding will support only as much voltage as comes from the IR drop and inductive reactance, which shouldn’t be more than a fraction of a volt. Nevertheless, I wound the core with transformer tape:

    FT82-43 toroid - wrapped
    FT82-43 toroid – wrapped

    That’s 3M 4161-11 electrical tape (apparently out of production, but perhaps equivalent to 3M’s Super 10 tape) cut into half-foot lengths, slit to 100 mils, and wrapped ever so gently.

    The thickest offering from the Big Box o’ Specialty Wire was 24 AWG, so that’s what I wound on it:

    FT82-43 toroid - wound
    FT82-43 toroid – wound

    That’s 56 turns, which should convert 2.2 A into 1000 G (enough to max out the Hall effect sensor) and is more in keeping with 24 AWG wire’s 3.5 A current rating.

    The insulated core requires just under 1 inch/turn, so figure the length at 56 inch. The wire tables show 26.2 Ω/1000 ft, so the DC winding resistance should be 120 mΩ. My desk meter has 0.1 Ω resolution, which is exactly the difference between shorted probes and probes across the coil: close enough.

    The inductance is 170 µH, so the inductive reactance at 120 Hz  = 128 mΩ.

    Now, for a bit of armor…

     

  • Bike Helmet Earbud Iteration

    Based on having to seal the rear vent hole of the previous earbud, I did the same for the new one:

    Earbud - blocked vent
    Earbud – blocked vent

    The audio quality was terrible, so I tried another bud with a foam windscreen over the hole and a hole punched in the middle of the double-sided white foam tape:

    Earbud - foam over vent
    Earbud – foam over vent

    The audio remained unintelligible, so I tried an upscale (but still cheap, because surplus) Koss earbud, first without blocking the vents and then with snippets of Kapton tape:

    Koss earbud - tape over vent
    Koss earbud – tape over vent

    The earphone has three slits on each side, but only the middle slit has a hole penetrating the case; it must be a stylin’ thing.

    That sounded better, so I’ll roll with it. There’s supposed to be a foam cover over the housing, but those things always get grody and fall off; there’s not much point.

    As nearly as I can tell, contemporary earbud designs optimize for volume (dBm/mV) and thumpin’ bass, all to the detriment of actual audio quality. Based on numerous samples over the years, there is zero correlation between price (admittedly, on the low end) and audio quality (admittedly, with my crappy hearing).

    I own a pair of very nice (and thoroughly obsolete) Shure E2c sound-isolating ear beetles that sound great (even with my crappy hearing), but I’m unwilling to chop them up for the bike headset …

  • Gapped Ferrite Toroid: 5 A Calculations

    Using a Hall effect sensor to report on the Kenmore 158’s universal motor current puts different limits on the ferrite toroid than the LED current sensor: higher current, bigger wires, and mandatory galvanic isolation. One could, of course, just buy an Allegro ACS713/4/5 (or whatever) sensor from, say, Digikey, but, for a one-off project, it’s more interesting to run the numbers and build the thing.

    The motor winding resistance limits the peak current to about 200 V / 40 Ω = 5 A, in the absence of the transistor current limiter, and, if it gets above that, things have gone very, very wrong. Mostly, I expect currents under 1 A and it may be useful to reduce the full scale appropriately.

    The cheap eBay “SS49” Hall effect sensors I’m using produce anywhere between 0.9 and 1.8 mV/G; I’ll use 1.4 mV/G, which is at least close to the original Honeywell spec. That allows a bit over ±1000 G around the sensor’s VCC/2 bias within its output voltage range (the original datasheet says minimum ±650 G), so I’ll use B = 1000 G as the maximum magnetic flux density. The overall calibration will be output voltage / input current and I’m not above doing a one-off calibration run and baking the constant into the firmware.

    The effective mean path length turns out to be a useful value for a slit toroid:

    effective MPL = (toroid MPL - air gap length) + (µ · air gap length)

    The SS49 style sensor spec says they’re 1.6 mm thick,  and the saw-cut gaps run a bit more, but 1.5 mm will be close enough for now.

    The relation between all those values:

    B = 0.4 π µ NI / (effective MPL)

    Solving for NI:

    NI = B · (eff MPL) / (0.4 π µ)

    Solving for N:

    N = B · (eff MPL) / (0.4 π µ I)

    You always round up the result for N, because fractional turns aren’t a thing you can do with a toroid.

    FT50-61 toroid:

    • µ = 125
    • Saturation B = 2350 G
    • MPL = 3.02 cm
    • Effective MPL = (3.02 – 0.15) + (125 · 0.15) = 21.6 cm
    • N = 28 turns

    A somewhat larger FT82-43 toroid:

    • µ = 850
    • Saturation B = 2750 G
    • MPL = 5.26 cm
    • Effective MPL = (5.26 – 0.15) + (850 · 0.15) = 133 cm
    • N = 25 turns

    The saturation flux density seems to be measured at H = 10 Oe, but that applies to the intact toroids. The air gap dramatically reduces the effective µ, so you must apply a higher H to get the same B in the ferrite at saturation. At least, I think that’s the way it should work.

    H = 0.4 π NI / (geometric MPL)

    Then:

    • FT50-61: H = 58 Oe
    • FT82-43: H = 30 Oe

    I’m surely missing some second-order effect that invalidates all those numbers.

    Figuring the wire size for the windings:

    FT50:

    • ID = 0.281 inch
    • Circumference = 0.882 inch
    • 28 turns → wire OD = 0.882/28 = 31 mil
    • 20 AWG without insulation

    FT82:

    • ID = 0.520 inch
    • Circumference = 1.63 inch
    • 25 turns → wire OD = 1.63/25 = 65 mil
    • 14 AWG without insulation

    Of course, the wire needs insulation, but, even so, the FT82 allows a more rational wire size.

    Page 4.12 of the writeup from Magnetics Inc has equations and a helpful chart. They suggest water cooling a diamond-bonded wheel during the slitting operation; my slapdash technique worked only because I took candy-ass cuts.

    A table of magnet wire sizes with varying insulation from Cooner Wire.

    Some general notes about building & measuring inductors from the University of Denver.

    Doodles for the FT82-43:

    FT82-43 Doodles
    FT82-43 Doodles

    Doodles for the FT50-61:

    FT50-61 Doodles
    FT50-61 Doodles

    Running the numbers using the Magnetics Inc equations:

    Ferrite Gap Doodles
    Ferrite Gap Doodles
  • Bike Helmet Boom Mic: Assembly

    After building the mic mount, another dab of epoxy mounted the length of AWG 10 wire I said I wouldn’t use:

    Bike Helmet Mic Boom - rod epoxy
    Bike Helmet Mic Boom – rod epoxy

    The whole point of the complex mount is to expose the two noise cancelling holes on the back of the electret element:

    Bike Helmet Mic - electret element rear
    Bike Helmet Mic – electret element rear

    Add heatstink tubing over the entire length of the boom wire, use more black cable ties, shape another foam ball:

    Bike Helmet Mic Boom - installed
    Bike Helmet Mic Boom – installed

    And it worked on the first try, not that there’s much to it.

    Yeah, that’s the HDR-AS30V camera mount up top: dork mode in full effect.

  • Kenmore 158: ET227 Transistor Drive Gain

    A closer look at the collector voltage and current for the brute-force ET227 NPN transistor motor drive:

    Model 158 - 77 mA base VCE 200 mA div
    Model 158 – 77 mA base VCE 200 mA div

    The motor current (200 mA/div) never goes to zero, but the ET227 collector voltage hits zero as the transistor saturates: the motor winding soaks up all the available line voltage and the transistor dissipation drops close to zero. The datasheet suggests VCE(sat) < 0.1 V for IC < 5 A, albeit with IB = 30 A (!).

    The ET227 base drive was 77 mA, measured on a better meter than the low-resolution one in the power supply, and the transistor gain works out to 8 = 620 mA / 77 mA along those flat tops.

    Eyeballometrically speaking, the dissipation averages 50 W = 90 V x 620 mA during those spiky sections where the transistor must absorb the difference between the line voltage and the motor voltage. The cursors say that takes 5 ms of the 8.3 ms period of the 120 Hz full wave rectified power, so the duty cycle is 42% and the average average dissipation works out to 20 W. That’s still enough to warm up that big heatsink; the motor driver will need a thermal sensor and a quiet fan.

    That commutation noise looks pretty scary, doesn’t it?

    The test setup:

    Kenmore 158 - AC motor FW ET227 drive - test setup
    Kenmore 158 – AC motor FW ET227 drive – test setup

    The bridge rectifier doesn’t really need a heatsink, but it looked better for a Circuit Cellar picture…

  • Flashlight Switch: Poor Solder Joints

    My desk flashlight has three “functions”:

    • 5 UV LEDs
    • 10 white LEDs
    • laser pointer

    A four-click rotary pushbutton switch actuates the three functions (plus “off”) in sequence:

    Flashlight switch - internal wiring
    Flashlight switch – internal wiring

    All three lights became intermittent, which suggested a poor return connection at the far end of the battery. The case is, of course, aluminum, with coarse-cut threads that grate as you tighten the parts. I cleaned the crud out of the threads, anointed them with Ox-Gard compound, and discovered that the laser and UV LEDs were still flaky.

    Taking the thing apart and unsoldering the switch connections revealed the problem:

    Flashlight switch - bad solder joints
    Flashlight switch – bad solder joints

    Yup, two lousy solder joints. They’re not exactly cold solder joints, because there’s not really a joint there to begin with; the switch tabs never got hot enough to bond with the molten solder before it cooled.

    A dab of flux and touch from a hot soldering iron solved that problem.

    Assemble in reverse order and it works better than it ever did before!