Inexpensive Mechanical Shutter and Driver for Optics ... - Raizen Lab
Inexpensive Mechanical Shutter and Driver for Optics ... - Raizen Lab
Inexpensive Mechanical Shutter and Driver for Optics ... - Raizen Lab
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<strong>Inexpensive</strong> <strong>Mechanical</strong><br />
<strong>Shutter</strong> <strong>and</strong> <strong>Driver</strong><br />
<strong>for</strong> <strong>Optics</strong> Experiments<br />
Todd P. Meyrath 1<br />
Atom <strong>Optics</strong> <strong>Lab</strong>oratory<br />
Center <strong>for</strong> Nonlinear Dynamics<br />
University of Texas at Austin<br />
c○ 2003 by Todd Meyrath<br />
May, 2003<br />
revised September 2003<br />
Here we give a simple mechanical shutter <strong>and</strong> driver design that is reliable, fast,<br />
<strong>and</strong> inexpensive (under $10 <strong>for</strong> a single shutter <strong>and</strong> driver). Complete schematics,<br />
PCB layouts, <strong>and</strong> parts list are given in the pages that follow. There are two basic<br />
versions given here which differ, principally, in the flag used to block the laser beam.<br />
The basic idea is straight<strong>for</strong>ward: an opaque flag is glued to a mechanical relay which<br />
moves into (or out of) the beam.<br />
Version 1: The flag is a small piece of folded aluminum foil which is glued to a small<br />
wire which is, in turn, glued to the top of the moving flat copper contact of the relay,<br />
see Figure 1. In test conditions given below, the per<strong>for</strong>mance of this relay is as follows:<br />
throw 2 mm<br />
closing velocity 1.7 mm/ms<br />
opening velocity 1.5 mm/ms<br />
time jitter ∼ 30µs<br />
Version 2: The flag is a piece of a steel razor blade (or a small cut mirror <strong>for</strong><br />
high power beams) that is attached with epoxy to a solid 14 gauge copper wire, see<br />
Figure 2. The extra length gives a much larger throw but the additional weight slows<br />
it down. In test conditions given below, the per<strong>for</strong>mance of this relay is as follows:<br />
throw 6.6 mm<br />
closing velocity 0.7 mm/ms<br />
opening velocity 0.5 mm/ms<br />
time jitter ∼ 30µs<br />
Definitions of the above: throw is the total distance that the flag moves, closing<br />
velocity is the velocity of the flag when the relay is being switched on, opening velocity<br />
1 Please send comments, questions, corrections, insults to meyrath@physics.utexas.edu<br />
1
is that when the relay is being switched off, jitter is the short time change in the<br />
response of the shutter. Of course, the ‘opening’ <strong>and</strong> ‘closing’ depends on where you<br />
place the beam. Here, we always assume that when the relay is switched on, the<br />
beam is blocked.<br />
Test: A 1 mm slit was cut into a sheet of paper which was placed directly behind<br />
the flag. This was then illuminated by a large beam of roughly uni<strong>for</strong>m intensity<br />
over the test area. The exiting light was detected with a high speed photodiode <strong>and</strong><br />
oscilloscope. The velocity was nearly constant over the range of 1 mm aperture of<br />
the test. The voltage used <strong>for</strong> this test was 20 V, see below. It was noted that speed<br />
increases with extra voltage, however, this was not quantified.<br />
Principle difficulty: The principle problem with a mechanical relay of this sort is<br />
that, without modification, the shutter bounces when the relay is released (<strong>for</strong> about<br />
10 to 20 ms in the case of version 2 - which has much worse bounce). It is simple to<br />
solve this issue by removing the upper contact of the relay <strong>and</strong> replacing it with a<br />
small piece of rubber sorbothane (www.sorbothane.com). In this case little bounce<br />
was observed in version 2, <strong>and</strong> none in version 1. In our BEC experiments, this<br />
problem presents no difficulty. Our pinciple application of these low cost shutters is<br />
<strong>for</strong> beams that are intensity controlled by AOMs. The AOMs do very fast switch<br />
off the beams with small leakage. The shutters described here are used to block the<br />
leakage <strong>for</strong> during the long time evaporative cooling. In this application, neither<br />
bounce nor timing is important. For this purpose, we used version 2 described here.<br />
This has the added advantage of a black guard region along the beam path. Version<br />
2 has also been used with a small cut silver mirror <strong>for</strong> beams with as much as 10 W<br />
of power. Removing the lower contact pin adds a small amount to the throw.<br />
On/Off delay: There is a delay in switching on <strong>and</strong> off of the shutter. The principle<br />
delays are due to position of the beam with respect to the flag <strong>and</strong> the speed of the<br />
relay. If the beam is very close to the flag, there will be a small delay <strong>for</strong> switching<br />
off (2 to 3 ms version 1, 4 to 5 ms version 2) <strong>and</strong> a longer <strong>for</strong> switching on (8 to 10 ms<br />
version 1, 12 to 15 ms) or vise versa. This was not studied in detail, except the jitter.<br />
<strong>Driver</strong> circuit: The relay used has a nominal switch voltage of 12 V. The more<br />
voltage the faster the shutter, within reason. Of course, one can not use a higher<br />
voltage then 25 V in the design shown – the voltage of the large capacitor. Another<br />
limit is the maximum gate-to-source voltage of the P-channel FET. We run at 20 V.<br />
The shutter is normally open <strong>and</strong> the driver circuit uses a MOSFET to switch the<br />
shutter off using a digital signal from a BNC which is not really necessary to be<br />
50 Ω, a 1 kΩ input resistance is listed. The basic philosophy of the circuit is that<br />
more current is required to close the shutter then to keep it closed. So current<br />
initially comes from the capacitor which is charged to the supply voltage, which<br />
gives current Iinit = Vsup/Rrelay. After the shutter is closed, current comes from<br />
the power supply, but the voltage across the relay coil is lower so the current is<br />
Iclosed = Vsup/(Rrelay + R3W). In our case, Vsup = 20 V, Rrelay = 155 Ω nominally,<br />
R3W = 400 Ω, so Iinit ∼ = 130 mA <strong>and</strong> Iclosed ∼ = 36 mA. Initially, the driver circuit<br />
supplies 2.6 W during the moment of relay closing <strong>and</strong> only 0.2 W while maintaining<br />
the relay in a closed position. This is power that does not end up on the optical<br />
table, which might have sensitivity to temperature drifts in beam paths. The power<br />
2
supply used is required to supply about 36 mA per shutter when closed. Otherwise it<br />
is recharging the capacitors through R3W. Although when closed, only about 1/2 W<br />
is burnt in R3W, a 3 W power resistor was used because the circuit may be used<br />
<strong>for</strong> many different types of relays (<strong>and</strong> the author’s original relay had a much lower<br />
resistance than the present one). The relay used is T90N1D12-12 from P&B Tyco<br />
electronics (www.tycoelectronics.com), it is soldered to a small PCB.<br />
Other designs: A different design <strong>for</strong> a low cost shutter is given in: Singer, et.<br />
al., Review of Scientific Instruments, Volume 73, pp. 4402, 2002. This design is<br />
based on a modified speaker <strong>and</strong> has slightly better specifications (same speed as<br />
version 1 with 5 mm throw). Singer’s design has the advantage of nearly the throw of<br />
version 2 presented here <strong>and</strong> the speed of version 1. However, Singer’s design has the<br />
disadvantage of unpleasant modifications to a speaker as well as lack on any st<strong>and</strong>ard<br />
part specification. The extra ef<strong>for</strong>t may be worthwhile if the improved throw is needed<br />
on the faster version 1. Our design has the advantage of extremely easy construction<br />
<strong>and</strong> little modification of widely available parts.<br />
Parts: The boards used are presensitized PCBs to be exposed with a fluorescent<br />
lamp, they were obtained from www.circuitspecialists.com. The layouts given were<br />
printed on overhead projector transparencies <strong>and</strong> the boards exposed with a simple<br />
fluorescent desk lamp <strong>for</strong> about 10 minutes. Most of the other parts were obtained<br />
from www.mouser.com.<br />
Parts <strong>for</strong> a single shutter <strong>and</strong> driver<br />
Quantity Part Manufacturer Description<br />
1 ZVP4424A Zetex P-channel MOSFET TO-92<br />
1 2N7000 On Semiconductor N-channel MOSFET TO-92<br />
1 RS-2B-400 Vishay Dale power resistor 400 Ω, 3 W<br />
1 T90N1D12-12 P&B Tyco electronics SPST PCB mount solenoid relay<br />
3 31-5538-10RFX Amphenol RF RA PCB mount BNC receptacle<br />
1 UPW1E102MHH Nichicon 1000µF, 25 V Electro. Capacitor<br />
1 SA30CA General Semiconductor 30 V Trans. Voltage. Suppressor<br />
1 GD101 Ever-Muse, 100x150mm double-sided PCB<br />
www.circuitspecialists.com<br />
1 GS101 Ever-Muse 100x150mm single-sided PCB<br />
1 1 kΩ 1/4 W resistor<br />
1 50 kΩ 1/4 W resistor<br />
Acknowledgements: The author would like to thank his co-workers on the <strong>Raizen</strong><br />
<strong>Lab</strong>’s rubidium BEC experiment: Florian Schreck, Jay Hanssen, <strong>and</strong> Chih-sung Chuu,<br />
<strong>and</strong> of course Prof. Mark <strong>Raizen</strong>.<br />
3
Upper contact pin removed<br />
rubber sheet added<br />
attached wire<br />
30 V TVS<br />
Aluminium Foil Flag<br />
Lower contact pin removed<br />
Relay moving contact<br />
mounting hardware<br />
T90N1D12-12<br />
Solenoid Relay<br />
BNC receptacle<br />
Figure 1: <strong>Shutter</strong> Version 1. The aluminum foil flag is attached to a small wire (cut<br />
resistor lead) which is attached to the relay’s moving contact, both with 5 minute<br />
epoxy. The upper <strong>and</strong> lower contact pins are easy to pull out be<strong>for</strong>e soldering. A<br />
small 1/16 inch thick rubber sorbothane sheet is attached to the top of relay’s moving<br />
contact by double sided tape.<br />
4
Hole <strong>for</strong> light<br />
30 V TVS<br />
solid 14 gauge wire<br />
Razor blade shutter<br />
Figure 2: <strong>Shutter</strong> Version 2. This version is basically the same as the previous where<br />
the flag attachment has been replaced by a much larger wire to add more throw. In<br />
this case, the flag is a piece of a steel razor blade that is attached with epoxy to a<br />
solid 14 gauge copper wire. In cases of high power beams, we have used a small cut<br />
silver mirror. Using the copper wire has the advantages of being pliable <strong>and</strong> can be<br />
placed to be normally open or closed, but has the disadvantage of added mass. The<br />
PCB <strong>and</strong> the flag were painted black <strong>for</strong> a reduction in scattered light. The hole can<br />
be made any size.<br />
5
Figure 3: <strong>Driver</strong> Circuit. Four channels shown: Digital in, Drive Out, ... It is<br />
suggested that box containing the circuit is carefully labeled with light <strong>and</strong> dark<br />
stripes over the digital <strong>and</strong> the drive BNC receptacles – this will help to avoid the<br />
obvious mistake which may damage the digital signal source.<br />
6
SOLENOID RELAY DRIVER<br />
Each Channel:<br />
1000μF<br />
25V<br />
+<br />
400Ω 3W<br />
ZVP4424A<br />
+Vsup (15V to 24V)<br />
S<br />
50kΩ<br />
to<br />
Solenoid<br />
S<br />
2N7000<br />
1kΩ<br />
Digital<br />
Input<br />
Todd Meyrath<br />
CNLD, Physics,<br />
Univ of Texas<br />
May 2003
Four Channel Solenoid <strong>Driver</strong> Layout<br />
Dig In 1<br />
50kΩ<br />
N-Chan<br />
S<br />
400Ω 3W<br />
3 circuits, 4 channels each<br />
Four Channel Solenoid <strong>Driver</strong> Todd Meyrath May 2003<br />
Dig In 1<br />
1kΩ<br />
50kΩ<br />
N-Chan<br />
S<br />
400Ω 3W<br />
D P-Chan<br />
+<br />
1000μF<br />
Dig In 2<br />
50kΩ<br />
1kΩ<br />
400Ω 3W<br />
Top<br />
D P-Chan 50kΩ D P-Chan 50kΩ<br />
D P-Chan<br />
GND<br />
+<br />
+ +<br />
1000μF<br />
Out 1 S Out 2 S Out 3 S Out 4<br />
Four Channel Solenoid <strong>Driver</strong> Todd Meyrath May 2003<br />
1kΩ<br />
D P-Chan<br />
+<br />
1000μF<br />
Dig In 2<br />
50kΩ<br />
1kΩ<br />
400Ω 3W<br />
Bottom<br />
+20V<br />
Dig In 3<br />
+20V<br />
1kΩ<br />
400Ω 3W<br />
D P-Chan 50kΩ D P-Chan 50kΩ<br />
D P-Chan<br />
GND<br />
+<br />
+ +<br />
1000μF<br />
Dig In 3<br />
Out 1 S Out 2 S Out 3 S Out 4<br />
Four Channel Solenoid <strong>Driver</strong> Todd Meyrath May 2003<br />
Dig In 1<br />
50kΩ<br />
N-Chan<br />
1kΩ<br />
S<br />
400Ω 3W<br />
D P-Chan<br />
+<br />
1000μF<br />
Dig In 2<br />
50kΩ<br />
1kΩ<br />
400Ω 3W<br />
+20V<br />
1kΩ<br />
400Ω 3W<br />
D P-Chan 50kΩ D P-Chan 50kΩ<br />
D P-Chan<br />
GND<br />
+<br />
+ +<br />
1000μF<br />
Dig In 3<br />
Out 1 S Out 2 S Out 3 S Out 4<br />
1kΩ<br />
400Ω 3W<br />
1000μF<br />
1000μF<br />
1000μF<br />
Dig In 4<br />
Dig In 4<br />
Dig In 4<br />
1kΩ<br />
1kΩ<br />
1kΩ<br />
400Ω 3W<br />
400Ω 3W<br />
400Ω 3W<br />
1000μF<br />
1000μF<br />
1000μF
Board Layout <strong>for</strong> 10 relay shutters<br />
Relay: T90N1D12-12 P&B Tyco Electronics<br />
Bottom<br />
Board Layout Version 1
Board Layout <strong>for</strong> 5 relay shutters<br />
Relay: T90N1D12-12 P&B Tyco Electronics<br />
Bottom<br />
Board Layout Version 2
Bottom