PSN-L Email List Message

Subject: Re: Seismograph pictures
From: Christopher Chapman chrisatupw@.......
Date: Sat, 11 Jun 2011 20:00:43 -0400 (EDT)


















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.pdf 
 
    The 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,
 
    Chris = Chapman   

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