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.

Tag: Sewing

Fabric arts and machines

  • 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…

     

  • 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
  • Kenmore 158: Pulley Form Tool FAIL

    Mulling over how to add a 1/rev sensor to the sewing machine motor, it occurred to me that simply drilling a hole through the pulley would provide a clean optical path and a convenient 2/rev output signal.

    However, the OEM pulley doesn’t extend beyond the end of the shaft:

    Kenmore 158 - AC drive motor - overview
    Kenmore 158 – AC drive motor – overview

    Rather than drill a hole in the shaft or (attempt to) affix something onto a pulley that spins at 10 kRPM, I figured I should make another pulley and mutilate that.

    Because this will surely call for more than one new pulley before I get everything right, a lathe form tool seemed in order. Introducing a suitable blank from the Bin o’ 1/4 Inch Bits to Mr. Bench Grinder produced a likely looking candidate, with an included angle of about 35° (a skosh over 17° on each side) and sized just a wee bit narrower than the pulley groove.

    From the top:

    Pulley form tool - top
    Pulley form tool – top

    From the side:

    Pulley form tool - side
    Pulley form tool – side

    Skim the surface of a 5/8 inch rod to match the pulley OD, plunge a cutoff tool to make most of the cut, insert bit in holder, align perpendicular to workpiece, line up to center of cut, slobber on more cutting lube:

    Pulley form tool - prepared blank
    Pulley form tool – prepared blank

    Plunging the tool slowly into the cut produces … no chips … nothing … smoke?

    Come to find out that the Bin o’ 1/4 Inch Bits contained not just lathe tool bits & blanks made from tool steel, but one length of 1/4 inch square key stock made from ordinary soft steel:

    Pulley form tool - damage
    Pulley form tool – damage

    I should have known that from the type of sparks flying off the grinding wheel, right?

    You knew that just from looking at the first picture, because a real lathe bit blank wouldn’t be all beat to shit…

    Drat!

  • Large Spool Adapter: Right-angle Version

    Mary recently learned that large spools of thread have a cross-wound lay that should feed over the end, not from the side as do ordinary stack-wound spools. So I built a right-angle adapter that fits over the not-quite-vertical spool pin on the sewing machine and aims directly at the thread tensioner:

    Large spool adapter - on sewing machine
    Large spool adapter – on sewing machine

    The solid model shows off the fluted rod that passes through the spool:

    Large Spool Adapter - solid model - mount
    Large Spool Adapter – solid model – mount

    It’s more impressive from the other end:

    Large Spool Adapter - solid model - spool end
    Large Spool Adapter – solid model – spool end

    The first pass at the rod had six flutes, but that seemed unreasonably fine; now it has four. The round base on the rod provides more griptivity to the platform while building and has enough space for the two alignment pins that position it in the middle of the dome:

    Large Spool Adapter - solid model - alignment holes
    Large Spool Adapter – solid model – alignment holes

    The dome gets glued to the rod base plate:

    Large spool adapter - clamped
    Large spool adapter – clamped

    The spool pin hole is a snug fit around the pin on the sewing machine, because otherwise it would tend to rotate until the spool pointed to the rear of the machine. The fluted rod is a snug friction fit inside the (cardboard) spool. Some useful dimensions:

    • Spool pin (on Model 158): 5 mm OD, 40 mm tall
    • Large spool cores: 16 mm ID, 27 mm OD, 70 mm long

    I had all manner of elaborate plans to make an expanding fluted rod, but came to my senses and built the simple version first. If that rod isn’t quite big enough, I can build another adapter, just like this one, only slightly larger. The source code includes a 0.5 mm taper, which may suffice.

    Back in the day, shortly after the Thing-O-Matic started producing dependable results, one of the very first things I made was a simple adapter to mount large spools on the pin in the most obvious way:

    Large spool adapter - old TOM version
    Large spool adapter – old TOM version

    Now we all know better than that, my OpenSCAD-fu has grown stronger, and the M2 produces precise results. Life is good!

    The OpenSCAD source code:

    // Large thread spool adapter
    // Ed Nisley - KE4ZNU - August 2014
    
    Layout = "Show";			// Build Show Spindle Spool
    
    Gap = 10.0;					// between pieces in 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
    
    LEN = 0;											// subscripts for cylindrical objects
    ID = 1;
    OD = 2;
    
    Spindle = [40.0,5.0,14.0];							// spool spindle on sewing machine
    Spool = [70.0,16.0,27.0];							// spool core
    
    Taper = 0.50;										// spool diameter increase at base
    
    CottonRoll = [65.0,Spool[OD],45.0];					// thread on spool
    
    Mount = [Spindle[LEN],(Spindle[ID] + 4*ThreadWidth),1.0*Spool[ID]];
    
    Flutes = 4;
    Flange = [2.0,Spool[OD],Spool[OD]];
    
    ScrewHole = [10.0,4.0 - 0.7,5.0];					// retaining screw
    
    PinOC = Spool[ID]/4;								// alignment pin spacing
    
    //----------------------
    // 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);
    
    }
    
    //- Locating pin hole with glue recess
    //  Default length is two pin diameters on each side of the split
    
    module LocatingPin(Dia=AlignPinOD,Len=0.0) {
    	
    	PinLen = (Len != 0.0) ? Len : (4*Dia);
    	
    	translate([0,0,-ThreadThick])
    		PolyCyl((Dia + 2*ThreadWidth),2*ThreadThick,4);
    
    	translate([0,0,-2*ThreadThick])
    		PolyCyl((Dia + 1*ThreadWidth),4*ThreadThick,4);
    		
    	translate([0,0,-(Len/2 + ThreadThick)])
    		PolyCyl(Dia,(Len + 2*ThreadThick),4);
    
    }
    
    //----------------------
    // Spindle 
    
    module SpindleMount() {
    
    	render(convexity=4)
    	difference() {
    		union() {
    			resize([0,0,Mount[OD]])							// spool backing plate
    				translate([0,CottonRoll[OD]/2,0])
    					sphere(d=CottonRoll[OD],center=true);
    			translate([0,CottonRoll[OD]/4,0])				// mounting post
    				rotate([90,0,0])
    					cylinder(d=Mount[OD],h=CottonRoll[OD]/2,center=true);
    		}
    		
    		translate([0,(2*Mount[LEN] - Protrusion),Mount[OD]/4])				// punch spindle hole
    			rotate([90,0,0])
    //				PolyCyl(Spindle[ID],2*Mount[LEN],6);
    				cylinder(d=Spindle[ID],h=2*Mount[LEN],$fn=6);
    				
    		for (i=[-1,1]) {									// punch alignment pin holes
    			translate([i*PinOC,CottonRoll[OD]/2,0])
    					LocatingPin(Len=Mount[OD]/3);
    		}
    				
    		translate([0,0,-CottonRoll[OD]])					// remove half toward spool
    			cube(2*CottonRoll[OD],center=true);
    	}
    
    }
    
    //----------------------
    // Spool holder
    
    module SpoolMount() {	
    
    	difference() {
    	
    		union() {
    				
    			translate([0,0,(Flange[LEN] - Protrusion)])
    				difference() {
    					cylinder(d1=(Spool[ID] + Taper),d2=Spool[ID],h=Spool[LEN],$fn=2*Flutes);						// fit spool ID
    					
    					for (a=[0 : 360/Flutes : 360-1])						// create flutes
    						rotate(a + 180/Flutes)
    							translate([Spool[ID]/2,0,-Protrusion])
    								rotate(180/16)
    								cylinder(r=Spool[ID]/4,h=(Spool[LEN] + 2*Protrusion),$fn=16);
    								
    					translate([0,0,(Spool[LEN] - ScrewHole[LEN])])			// punch screw hole
    						PolyCyl(ScrewHole[ID],(ScrewHole[LEN] + Protrusion),6);
    
    				}
    			cylinder(d=Flange[OD],h=Flange[LEN]);							// base flange
    		}
    		
    		for (i=[-1,1])												// punch alignment pin holes
    			translate([0,i*PinOC,0])								//  ... orients solid flange up
    					LocatingPin(Len=Flange[LEN]);	
    	}
    
    }
    
    
    ShowPegGrid();
    
    if (Layout == "Spindle") {
    	SpindleMount();
    }
    if (Layout == "Spool") {
    	SpoolMount();
    }
    
    if (Layout == "Show") {
    	translate([0,Mount[OD]/4,2.0]) {
    		rotate([90,0,0])
    			SpindleMount();
    		translate([0,Gap,CottonRoll[OD]/2])
    			rotate([-90,0,0]) rotate(90)
    				SpoolMount();
    	}
    	color("Orange") {
    		translate([0,0,2])
    			cylinder(d=Spindle[ID],h=Spindle[LEN],$fn=6);
    		cylinder(d=Spindle[OD],h=2.0,$fn=18);
    	}
    		
    }
    
    if (Layout == "Build") {
    	translate([-5,0,0])
    		rotate(90)
    			SpindleMount();
    	translate([Flange[OD]/2,0,0])
    			SpoolMount();
    }
    
  • 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…

  • Image File Recovery Redux

    Took a picture of the sewing machine setup with the Sony DSC-F717, transferred it into DigiKam, got the “done transferring, you can disconnect the camera” message, believed it, disconnected the camera, deleted the image file, and then discovered that DigiKam mislaid the image file.

    Rather than re-set-up and re-take the shot, I followed my own directions and recovered the image from the Memory Stick:

    dmesg | tail
    [43176.079853] usb 2-1.6.3: New USB device strings: Mfr=1, Product=2, SerialNumber=0
    [43176.079855] usb 2-1.6.3: Product: Sony PTP
    [43176.079856] usb 2-1.6.3: Manufacturer: Sony
    [43198.073652] usb 2-1.6.3: USB disconnect, device number 22
    [43333.788533] sd 9:0:0:0: [sdc] 1947648 512-byte logical blocks: (997 MB/951 MiB)
    [43333.803292] sd 9:0:0:0: [sdc] No Caching mode page found
    [43333.803299] sd 9:0:0:0: [sdc] Assuming drive cache: write through
    [43333.824681] sd 9:0:0:0: [sdc] No Caching mode page found
    [43333.824688] sd 9:0:0:0: [sdc] Assuming drive cache: write through
    [43333.825491]  sdc: sdc1
    sudo dd if=/dev/sdc of=/tmp/pix.bin bs=1M
    ^C615+0 records in
    614+0 records out
    643825664 bytes (644 MB) copied, 38.5841 s, 16.7 MB/s
    strings -t x pix.bin | grep Exif | head
      68006 Exif
     208006 Exif
     3f8005 _Exif
     7b8006 Exif
    13d8006 Exif
    15b0005 wExif
    1798005 CExif
    19c0006 Exif
    1b90006 Exif
    1f98005 %Exif
    dd if=pix.bin of=image03.jpg bs=$((16#1000)) count=1K skip=$((16#3f8))
    1024+0 records in
    1024+0 records out
    4194304 bytes (4.2 MB) copied, 0.0121431 s, 345 MB/s
    display image03.jpg
    convert image03.jpg dsc00656.jpg
    

    Obviously, there was a bit more flailing around than you see here, but that’s the gist of the adventure. For what it’s worth, image01 was a random blurred shot and image02 is the ID picture I keep on all my cameras.

    The convert step discards all the junk after the end of the image, so the dsc00656.jpg file doesn’t include anything unexpected.

    The picture isn’t all that much to look at, even after cropping out the background, but …

    Kenmore 158 - stepper drive test
    Kenmore 158 – stepper drive test

    The advantage of the manual method: renewing one’s acquaintance with tools that come in handy for other tasks.