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Student Report (National Research Council of Canada. Institute for Ocean Technology); no. SR-2006-12, 2006

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Ice detection tripod modification, 2006

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DOCUMENTATION PAGE

REPORT NUMBER SR-2006-12

NRC REPORT NUMBER DATE April 2006 REPORT SECURITY CLASSIFICATION

unclassified

DISTRIBUTION unlimited TITLE

Ice Detection Tripod Modification, 2006

AUTHOR(S) T.Osmond

CORPORATE AUTHOR(S)/PERFORMING AGENCY(S)

National Research Council – Institute for Ocean Technology PUBLICATION

SPONSORING AGENCY(S)

IOT PROJECT NUMBER 42_2096_10

PAGES 5 KEY WORDS

Tripod, Ice Detection

APP. A-D FIGS. 1 TABLES 0 SUMMARY

This document outlines the design work completed as modifications to one of the new QuickSet Hercules tripods and tripod heads purchased by the Institute for Ocean Technology. These modifications will be implemented as part of the readiness design modifications in preparing one of the tripods for the IOT Ice Detection project 42_2096_10. The design work consists of attaching two potentiometers to the pan and tilt axes of the tripod so that pan and tilt angles may be measured.

ADDRESS National Research Council Institute for Ocean Technology Arctic Avenue, P. O. Box 12093 St. John's, NL A1B 3T5

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National Research Council Conseil national de recherches Canada Canada Institute for Ocean Institut des technologies Technology océaniques

ICE DETECTION TRIPOD MODIFICATION, 2006

SR-2006-12

T. Osmond

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Quickset Tripod Head Design Modifications

The purpose of this design modification is to attach potentiometers to the Quickset tripod head so that changes in pan and tilt angles may be read and accurately measured by a computer.

Potentiometer Selection

Experimentation and analysis into three different potentiometers yielded the results contained under CAD_User\Projects\42_2096 Ice

Detection\TOsmond\Pot Linearity.xls.

The data from these experiments are contained in Appendix A. The potentiometers tested were (for data sheets see Appendix B): A Bourns 3540,

A Bourns 6534,

And A Vishay Spectrol 157.

Two experiments were conducted on each potentiometer, fine linear measures and full range linear measurements. The same apparatus was used for both experiments. A dial was attached to the potentiometer and a quadrant encircled the potentiometer. In this way angle readings could be taken from visually from the quadrant. The potentiometer being tested was connected to a multimeter accurate to four decimal places and set to read voltage (see Figure 1). For fine linear measurements the voltage output of each potentiometer was measured over a range of seven degrees. Readings were taken at 1/3rd of a degree intervals for a total of 21 readings each trial. Each potentiometer was tested three times.

For the full range linear measurements six to ten readings were taken of each potentiometer voltage over the full range of the individual potentiometer. Intervals were different because the full range of each of the potentiometers is different. Again three trial measurements were taken for each potentiometer. All data was analyzed in Microsoft Excel.

The three potentiometers were selected for testing based on availability from the electronics department. Data analysis following testing and consultation with Dr. Robert Gagnon decided the Vishay Spectrol 157 to yield the most accurate and predictable results. This potentiometer was selected to measure the angles in both pan and tilt. This potentiometer also carries the advantage of being capable full 360o travel without failing although the potentiometer has a dead band

between 340o and 360o. This removes the risk of damaging the potentiometer by over-rotating it.

Following selection of the potentiometer to be used more extensive testing was conducted to gain a more accurate understanding of the linear characteristics of the piece of equipment. This involved taking voltage readings at 18 locations

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over the full range of the potentiometer over a series of five test trials. The results from these experiments are also contained in Appendix A.

Experimentation has indicated that the Vishay Spectrol 157-11/03 potentiometer displays linear characteristics with variation following a fourth power curve. Measured to this curve we have an accuracy of within approximately 10 ohms over a range of 300 degrees. This curve yields an error of approximately 0.35 degrees.

Though all potentiometers will have a different error in linearity the potentiometer we tested followed a linear profile of y = 7E-11x4 - 5E-09x3 - 2E-05x2 + 0.0303x + 0.0363. Readings were taken every 20 degrees and the change in resistance or increase in resistance over 20 degrees was found to follow the curve y = -8E-08x4 + 6E-05x3 - 0.0161x2 + 1.0532x + 548.98. In both cases fourth order polynomials were found to follow the data most accurately checking trends up to the sixth order polynomial as available in Microsoft Excel.

Looking at using brass gears from the available selection on

www.smallparts.com.

Brass Spur Gears – 32 pitch 20o pressure angle.

http://www.smallparts.com/products/descriptions/gbs.cfm shows a table of gear selections (see also Appendix C).

The 1” gear GBS – 3232 is the smallest gear that will fit our potentiometer with no machining necessary. This attributed to the gear bore of 0.25” and the

potentiometer shaft diameter of 0.249”. This gear will be used in both pan and tilt applications.

Tilt Gearing

For this axis we need at least 90 degrees rotation. We can use up to 300

degrees on the potentiometer. Thus our maximum gear ratio must be 300/90 = 3.33:1. Using our available gear ration of 3:1 we will use a range of 270 degrees rotation of the potentiometer. This will yield a maximum resolution of 0.117 degrees.

Potentiometer pinion – 1” GBS – 3232 Tripod gear – 3” GBS – 3296

This gear will be mounted on the non-toothed side of tripod head and the potentiometer will attach to the base of the head (see drawing 2096U01 – Appendix D).

Pan Gearing

For this axis we need at least 180 degrees rotation. We can use up to 300

degrees on the potentiometer. Thus our maximum gear ratio must be 300/180 = 1.67:1. Using our available gear ration of 1.5:1 we will use a range of 270

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degrees rotation of the potentiometer. This will yield a maximum resolution of 0.233 degrees.

Potentiometer pinion – 1” GBS – 3232 Tripod gear – 1.5” GBS – 3248

This gear will mount within the center of the tripod and the potentiometer will attach to the base of the head (see drawing 2096U02 – Appendix D).

Modifications and Design

Several modifications to the tripod are necessary. A number of unique pieces are to be fabricated by the Institute. These drawings are available under file: CAD_User\Projects\42_2096 Ice Detection\Tosmond\Tripod.ckd and is contained in Appendix D

Tilt Bracket Modification

One small modification is necessary for the Tilt Bracket. A ¼-20 hole must be drilled and tapped through the tilt axis on one side. It is imperative that this hole be dead center of the tilt axis (see drawing 2096U04 – Appendix D).

Base Modification

In order to attach a gearing system to the tilt access several modifications are necessary. First of all a potentiometer mount must be attached to the base. Two clearance holes must be drilled through the side of the base to pass through two ¼-20 bolts (see drawing 2096U04 – Appendix D).

Tilt Measurements

A potentiometer is mounted to the base of the tripod head and a gear is attached to the potentiometer. A pinion is fitted to a shafted that has been screwed into the hole in the tilt axis. The tilting of the head will cause the gear to turn the pinion and the potentiometer reads the angle of tilt when properly calibrated. Pan Measurements

A 3/8” bolt holds the tripod head to the tripod. This bolt sets the pan axis and it is to this bolt that the shaft of the central pan gear will attach. The design proposes a drilled and tapped hole to penetrate the bolt, tapped for an 8-32 UNC-2B

thread. A shaft with a threaded end will screw into the bolt passing through the center gear. Mating with that gear is a pinion. The pinion is mounted to the tripod head base using pre-existing threaded holes.

Rough Design

The design of the potentiometer mounts have been made according to rudimentary measurement methods and the accuracy is low in the wake of

unavailable drawings from the fabricator. Therefore it is likely that both mounting blocks may require further adjustments in the form of, but not limited to, removing or adding material to certain surfaces and repositioning drilled holes. These

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terms are in reference to the fabrication drawings 2096U13 & 2096U14 (see Appendix D).

Conclusions

Bar some minor adjustments, the design for attaching the potentiometers to both the pan and tilt axes should provide smooth and accurate measurements. This design is to be implemented into one tripod only, that is the tripod holding the telescope. Maximum accuracies have been given above for the potentiometers including increased resolution due to gear ratios. Obviously these accuracies will not be achieved due to imperfections in fabrication and unavoidable backlash in the gears*. With careful and precise fabrication an inaccuracy of 0.3-0.5 degrees may be expected.

Figures

Figure 1 – Potentiometer Measuring Apparatus

*

A more accurate device has been purchased to offer remote control of the laser. This device would also be useful for controlling the telescope should the potentiometer calibration and accuracy prove to be insufficient for this project application.

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Appendices

Appendix A – Experimental Data Appendix B – Data Sheets

Appendix C – Gear Selection Table Appendix D – Modification Drawings

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Figure

Figure 1 – Potentiometer Measuring Apparatus

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