Randall Pratt rpratt@............. Sent: Fri, 3 Jun 2011 17:20 Subject: Seismograph pictures Here are links to a couple pictures of the latest incarnation of my continu= ing experiment in recycling. http://mit.midco.net/rpratt/images/Vertical.J= PG I started with optical position sensing and moved to different coil a= nd damping configurations. The upper spring attachment is adjustable over = about 4" in out up down. The attachment to the carbon fiber boom was also i= nitially adjustable but is now in place for the current 2.68 second period.= I have experimented with periods of 1 to 4.5 seconds. I cast the lead ma= ss which has the vertical damping vane integral and a brass bolt threaded i= nto it for fine balance adjustments. http://mit.midco.net/rpratt/images/Coi= lDamp.JPG Damping is adjustable by turning the damping magnets on threaded= attachment bolts to set the gap between the 2 sides. I tried a knife edge= pivot and found it basically worthless so now have a flex pivot in compres= sion. The main frame is 3/16" by 1 1/2" steel angle brazed together. The = magnet has an extension to the center pole into the coil and the outer pole= face is removed to prevent shortcut of field below the coil. =20 =20 I like the steel angle construction for simplicity and quick assembly. I l= ike the damping system as the force lines are not offset and damping is eas= ily tuned to a fine level and not easily bumped out of adjustment. The dam= ping system is also fixed to the frame so it does not pick up separate vibr= ations. The solenoid type coil set up is very sensitive. The change from = knife edge to flex is a must for anyone contemplating construction. In the= future I may try the optical position system as a feedback loop but it did= not compare in sensitivity to the coil.=20 =20 Hi Randall, =20 Congratulations on completing a successful project!=20 =20 To eliminate any sensitivity to horizontal motion, the centre of gravit= y of the arm needs to be at the same vertical position as the flex suspensi= on. The arm needs to be ~horizontal. =20 You can also make a very satisfactory frame by BOLTING L section mild s= teel together! For a Lehman I used a 12" cross bar, 1" x 1 3/8" L section, = with two level adjust bolts at the ends. Two 30" horizontal L bars with a s= ingle 5" cross bar on the end with a third level adjust bolt at it's centre= , to hold the magnet blocks etc. Two 18" vertical L bars with a 4.75" top b= ar and a 4.5" lower cross bar to support the boom bearing. Connect two 13" = diagonal 1" x 1" L barsat 45 degrees between the upright and the horizontal= frames to cross brace them. =20 I agree with your finding that a real knife edge does NOT give a satisf= actory bearing. Neither does the point in a cup arrangement. I wonder if so= me guy years ago didn't realise that the "knife edge bearings" used in chem= ical balances are in reality tiny cylinders? =20 What material / dimensions did you use for the flexures under compression, = please?=20 Have you tried an old fashioned twin edged safety razor blade? You clamp on= e blade to the arm and the other to the upright. The two U loops at the end= s of the blade do the flexing. They are about 3.7 thou" thick, 0.14" wide a= nd 0.28" long. You can easily narrow the width using a small carbide cuttin= g disk in a drill.=20 Two other high load bearing types which DO work well are a plane rollin= g on a sphere and crossed circular section rods. You can buy tungsten carbi= de balls (www.smallparts.com) and solid triangular lathe tool flats, but a = stainless steel scalpel blade rolling on a stainless steel ball bearing is = much cheaper < $2! The SEPUK uses crossed tungsten carbide needle rollers S= ee http://www.mindsetsonline.co.uk/images/Seismometer.pdf=20 =20 The way you can increase the period of a vertical seismometer is to red= uce the angle the spring makes with the horizontal arm and mount the top at= tachment FURTHER BEHIND the vertical pillar. This increases the tension in= the spring. Extension springs have a natural zero tension length. This may= be measured by measuring the tension in the spring at two lengths, plottin= g them on a graph and measuring the zero intercept. If you run the system w= ith a "zero length" spring, theoretically you get an infinite period, but w= ith a steel spring the system will be unstable and it may collapse as the t= emperature increases. An 8 second period is about the best that you can hop= e for. Amateur constructors can use a period compensation amplifier to reco= ver signals from up to 10x the natural period. =20 There are two problems with using ferrite magnets. The saturation field= is relatively low and it is also quite strongly temperature dependant. Thi= s requires the use of rather large damping plates and sensor coils. Efficie= nt dampers and sensors using NdFeB magnet quads are described at www.jclahr= ..com/science/psn/chapman The very sensitive rectangular coils use only abou= t 2,000 turns! Using pairs of flat rectangular magnets removes the requirem= ent for having a magnetic return path through the mounting frame. =20 You can use optical sensing quite easily, but the system needs to be co= rrectly designed using large area photo diodes and a very stable light sour= ce. Tungsten filament bulbs run at about 3/4 their rated voltage, are excel= lent. You can use Infra Red LEDs with metal cases, but you do need to stabi= lise their temperature, since the photo output is strongly temperature depe= ndant.=20 I have used BPW34 photo diodes for a +/-1 mm range and my photo amplifi= er circuit is shown on the above website. The noise level was about 14 nano= metres. You need to run the photo diodes at about 50 to 100 micro amps. Th= e practical limit is provided by the photon noise. For a total sample charg= e of N electrons, the noise is SQRT(N). The charge on a single electron is= 1.602^-19 coulombs and 1 coulomb / second =3D 10 amps. You can also buy lo= ng narrow photo diodes more suitable for a Lehman. =20 Have fun! =20 Regards,=20 =20 Chris Chapman =20= Randall Pratt rpratt@.............
Sent: Fri, 3 Jun 2011 17:20
Subject: Seismograph pictures
Here are links to= a couple pictures of the latest incarnation of my continuing experiment in= recycling. http://mit.midco.net/rpratt/images/Vertical.JPG &nbs= p; I started with optical position sensing and moved to differen= t coil and damping configurations. The upper spring attachment is adj= ustable over about 4" in out up down. The attachment to the carbon fiber bo= om was also initially adjustable but is now in place for the current 2.68 s= econd period. I have experimented with periods of 1 to 4.5 seconds.&n= bsp; I cast the lead mass which has the vertical damping vane integral and = a brass bolt threaded into it for fine balance adjustments. http://mit.mid= co.net/rpratt/images/CoilDamp.JPG Damping is adjustable by turnin= g the damping magnets on threaded attachment bolts to set the gap between t= he 2 sides. I tried a knife edge pivot and found it basically worthle= ss so now have a flex pivot in compression. The main frame is 3/16" b= y 1 1/2" steel angle brazed together. The magnet has an extension to = the center pole into the coil and the outer pole face is removed to prevent= shortcut of field below the coil.I like the steel = angle construction for simplicity and quick assembly. I like the damp= ing system as the force lines are not offset and damping is easily tuned to= a fine level and not easily bumped out of adjustment. The damping sy= stem is also fixed to the frame so it does not pick up separate vibrations.= The solenoid type coil set up is very sensitive. The change fr= om knife edge to flex is a must for anyone contemplating construction. = ; In the future I may try the optical position system as a feedback loop bu= t it did not compare in sensitivity to the coil.&nb= sp;Hi Randall,Congra= tulations on completing a successful project!To eli= minate any sensitivity to horizontal motion, the centre of gravity of the a= rm needs to be at the same vertical position as the flex suspension. The ar= m needs to be ~horizontal.You ca= n also make a very satisfactory frame by BOLTING L section mild steel = together! For a Lehman I used a 12" cross bar, 1" x 1 3/8" L section, = with two level adjust bolts at the ends. Two 30" horizontal L bars with a s= ingle 5" cross bar on the end with a third level adjust bolt at it's centre= , to hold the magnet blocks etc. Two 18" vertical L bars with a 4.75" top b= ar and a 4.5" lower cross bar to support the boom bearing. C= onnect two 13" diagonal 1" x 1" L barsat 45 degrees between the uprigh= t and the horizontal frames to cross brace them.I= agree with your finding that a real knife edge does NOT give a satisfactor= y bearing. Neither does the point in a cup arrangement. I wonder if some&nb= sp;guy years ago didn't realise that the "knife edge bearings" used in chem= ical balances are in reality tiny cylinders?What material / dimension= s did you use for the flexures under compression, please?Have you tried an old fas= hioned twin edged safety razor blade? You clamp one blade to the arm and th= e other to the upright. The two U loops at the ends of the blade do the fle= xing. They are about 3.7 thou" thick, 0.14" wide and 0.28" long. You can ea= sily narrow the width using a small carbide cutting disk in a drill.Two ot= her high load bearing types which DO work well are a plane rolling on = a sphere and crossed circular section rods. You can buy tungsten carbide ba= lls (www.smallparts.com) and sol= id triangular lathe tool flats, but a stainless steel scalpel blade ro= lling on a stainless steel ball bearing is much cheaper < $2! The SEPUK = uses crossed tungsten carbide needle rollers See http://www.mindsetsonline.co.uk/im= ages/Seismometer.pdfThe wa= y you can increase the period of a vertical seismometer is to reduce the an= gle the spring makes with the horizontal arm and mount the top attachment F= URTHER BEHIND the vertical pillar. This increases the tension in the = spring. Extension springs have a natural zero tension length. This may be m= easured by measuring the tension in the spring at two lengths, plotting the= m on a graph and measuring the zero intercept. If you run the sys= tem with a "zero length" spring, theoretically you get an infinite period, = but with a steel spring the system will be unstable and it may collapse as = the temperature increases. An 8 second period is about the best that you ca= n hope for. Amateur constructors can use a period compensation amplifier to= recover signals from up to 10x the natural period.There = are two problems with using ferrite magnets. The saturation field is relati= vely low and it is also quite strongly temperature dependant. This req= uires the use of rather large damping plates and sensor coils. Efficie= nt dampers and sensors using NdFeB magnet quads are described at www.jclahr.com/science/psn/chap= man The very sensitive rectangular coils use only about 2,000= turns! Using pairs of flat rectangular magnets removes the requirement for= having a magnetic return path through the mounting frame.You ca= n use optical sensing quite easily, but the system needs to be correctly de= signed using large area photo diodes and a very stable light source. T= ungsten filament bulbs run at about 3/4 their rated voltage, are excellent.= You can use Infra Red LEDs with metal cases, but you do need to stabilise = their temperature, since the photo output is strongly temperature depe= ndant.I have= used BPW34 photo diodes for a +/-1 mm range and my photo amplifier ci= rcuit is shown on the above website. The noise level was about 14 nano metr= es. You need to run the photo diodes at about 50 to 100 micro amps. The pra= ctical limit is provided by the photon noise. For a total sample charge of = N electrons, the noise is SQRT(N). The charge on a single electron is= 1.602^-19 coulombs and 1 coulomb / second =3D 10 amps. You can also buy lo= ng narrow photo diodes more suitable for a Lehman.Have f= un!Regards, = div>Chris = Chapman[ Top ] [ Back ] [ Home Page ]