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'''Teledeltos paper''' is an electrically [[conductive]] paper. It is formed by a coating of [[carbon]] on one side of a sheet of [[paper]], giving one black and one white side.


It has several uses within engineering, usually for modelling the distribution of [[electric field|electric]] and other [[scalar field]]s.


== Use ==
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Teledeltos provides a sheet of a uniform resistor, with [[isotropic]] [[resistivity]] in each direction. As it is cheap<ref >{{Cite web
  |title=Teledeltos conductive paper sheets
  |url=http://www.timstar.co.uk/Search/1/12/0/teledeltos/NA/Best.html
}}</ref> and easily cut to shape, it may be used to make one-off resistors of any shape needed. The paper backing also forms a convenient insulator from the bench. These are usually made to represent or model some real-world example of a two-dimensional [[scalar field]], where is it is necessary to study the field's distribution. This field may be an electric field, or some other field following the same linear distribution rules.
 
The resistivity of Teledeltos is around 6 kilohms / square.<ref name="Baxter" /><ref group="note" >Note that the [[sheet resistance|resistivity units for a two-dimensional sheet]] are ohms / square (<math>\Omega/\Box</math>), not the [[mho]]s or [[Siemens (unit)|Siemens]] that would be used for a bulk resistor.</ref> This is low enough that it may be used with safe low voltages, yet high enough that the currents remain low, avoiding problems with [[contact resistance]].
 
Connections are made to the paper by painting on areas of silver-loaded [[conductive paint]] and attaching wires to these, usually with spring clips.<ref name="Baxter" /><ref name="Aston" >{{Cite web
  |title=Field Plotting Using Teledeltos Paper
  |publisher=Department of Electronic Engineering and Applied Physics, Aston University
  |url=http://www-users.aston.ac.uk/~pearcecg/Teaching/PDF/TELDELT.PDF
  |format=pdf
}}</ref> Each painted area has a low resistivity (relative to the carbon) and so may be assumed to be at a constant voltage. With the voltages applied, the current flow through the sheet will emulate the field distribution. Voltages may be measured within the sheet by applying a voltmeter probe (relative to one of the known electrodes) or current flows may be measured. As the sheet's resistivity is constant, the simplest way to measure a current flow is to use a small two-probe voltmeter to measure the voltage difference between the probes. As their spacing is known, and the resistivity, the resistance between them and (by [[Ohm's law]]) the current flow can be easily determined.
 
An assumption in some cases is that the surrounding field is 'infinite', this would also require an infinite sheet of Teledeltos. Provided that the sheet is merely 'large' in comparison to the experimental area, a sheet of finite size is sufficient for most experimental practice.<ref name="Aston" />
 
== Field plotting ==
The basic technique for plotting a field is to first construct a model of the [[independent variable]]s, then to use voltage meter probes to measure the [[dependent variable]]s. Typically this means applying known voltages at certain points, then measuring voltages and currents within the model. The two basic approaches are to either applying electrodes and a voltage at known points within a large sheet of Teledeltos (modelling an infinite field) or else to cut a shape from Teledeltos and then apply voltages to its edges (modelling a bounded field).<ref name="Baxter" /><ref name="Aston" /> There is a common practical association that electrical field models are usually infinite and thermal models are usually bounded.
 
== Modelling fields by analogy ==
Although the modelling of electric fields is itself directly useful in some fields such as [[thermionic valve]] design,<ref name="Pease" >{{Cite web
  |title=What's All This Teledeltos Stuff, Anyway?
  |url=http://electronicdesign.com/article/analog-and-mixed-signal/what-s-all-this-teledeltos-stuff-anyway-12594
  |date=30 May, 1994
  |author=Bob Pease
}}</ref> the main practical use of the broader technique is for modelling fields of other quantities. This technique may be applied to ''any'' field that follows the same linear rules as Ohm's law for bulk resistivity. This includes heat flow, some optics and some aspects of Newtonian mechanics. It is not usually applicable to fluid dynamics, owing to viscosity and compressibility effects, or to high-intensity optics where [[non-linear optics|non-linear effects]] become apparent. It may be applicable to some mechanical problems involving homogeneous and isotropic materials such as metals, but not to composites.
 
Before the use of Teledeltos, a similar technique had been used for modelling gas flows, where a shallow tray of [[copper sulphate]] solution was used as the medium, with copper electrodes at each side. Barriers within the model could be sculpted from wax. Being a liquid, this was far less convenient. [[Stanley Hooker]] describes its use pre-war, although he also notes that [[compressibility]] effects could be modelled in this way, by sculpting the base of the tank to give additional depth and thus conductivity locally.<ref >{{Cite book
  |last=Hooker |first=Stanley |authorlink=Stanley Hooker
  |title=Not much of an engineer. An autobiography
  |publisher=Airlife Publ.  |location=Shrewsbury
  |year=2002
  |isbn=1-85310-285-7
  |ref=harv
  |pages=9–10
}}</ref>
 
One of the most important applications is for thermal modelling. Voltage is the analog of temperature and current flow that of [[heat flow]]. If the boundaries of a [[heatsink]] model are both painted with conductive paint to form two separate electrodes, each may be held at a voltage to represent the temperatures of some internal heat source (such as a microprocessor chip) and the external ambient temperature. Potentials within the heatsink represent internal temperatures and current flows represent heat flow. In many cases the internal heat source may be modelled with a [[constant current source]], rather than a voltage, giving a better analogy of power loss as heat, rather than assuming a simple constant temperature. If the external airflow is restricted, the 'ambient' electrode may be subdivided and each section connected to a common voltage supply through a resistor or current limiter, representing the proportionate or maximum heatflow capacity of that airstream.  
 
As heatsinks are commonly manufactured from [[aluminium extrusion|extruded aluminium section]]s, the two-dimensional paper is not usually a serious limitation. In some cases, such as pistons for internal combustion engines, three dimensional modelling may be required. This has been performed, in a manner analogous to Teledeltos paper, by using volume tanks of a conductive electrolyte.<ref >{{Cite journal
  |title=The Napier Deltic Diesel Engine in Main-line Locomotives
  |journal=Proc. Inst. Mech. Engrs.
  |last=Chamberlin
  |first=R.H.
  |year=1963–1964
  |volume=178
  |issue=3
  |ref={{harvid|Chamberlin}}
  |page=66
  |url=http://pcp.sagepub.com/content/178/11/53.full.pdf+html
}}</ref>
 
This thermal modelling technique is useful in many branches of [[mechanical engineering]] such as heatsink or [[radiator]] design and [[die casting]].<ref name="jorstad" >{{Cite journal
  |last = John L.  |first = Jorstad
  |title = Aluminum Future Technology in Die Casting
  |pages = 19
  |url = http://www.wpi.edu/Images/CMS/MPI/Jorstad.pdf
  |journal = Die Casting Engineering
  |year = 2006  |month = September
  |archiveurl = http://www.webcitation.org/5uBp7JOJZ  |archivedate = 11-12-2010
}}</ref>
 
The development of [[computational modelling]] and [[finite element analysis]] has reduced the use of Teledeltos, such that the technique is now obscure and the materials can be hard to obtain.<ref name="Baxter" /> Its use is still highly valuable in teaching, as the technique gives a very obvious method for measuring fields and offers immediate feedback as the shape of an experimental setup is changed, encouraging a more fundamental understanding.<ref name="Aston" /><ref name="Pease" />
 
== Sensors ==
Teledeltos can also be used to make [[sensor]]s, either directly as an embedded resistive element or indirectly, as part of their design process.
 
=== Resistive sensors ===
A piece of Teledeltos with conductive electrodes at each end makes a simple [[resistor]]. Its resistance is slightly sensitive to applied mechanical [[strain (mechanics)|strain]] by bending or compression, but the paper substrate is not robust enough to make a reliable sensor for long-term use.
 
A more common resistive sensor is in the form of a [[potentiometer]]. A long, thin resistor with an applied voltage may have a conductive probe slid along its surface. The voltage at the probe depends on its position between the two end contacts. Such a sensor may form the keyboard for a simple electronic musical instrument like a [[Tannerin]] or [[Stylophone]].
 
A similar linear sensor uses two strips of Teledeltos, placed face to face. Pressure on the back of one (finger pressure is enough) presses the two conductive faces together to form a lower resistance contact. This may be used in similar potentiometric fashion to the conductive probe, but without requiring the special probe. This may be used as a classroom demonstration for another electronic musical instrument, with a [[ribbon controller]] keyboard, such as the [[Korg Monotron|Monotron]].  If crossed electrodes are used on each piece of Teledeltos, a two-dimensional [[Touchscreen#Resistive|resistive touchpad]] may be demonstrated.
 
=== Capacitive sensors ===
Although Teledeltos is not used to manufacture capacitive sensors, its field modelling abilities also allow it to be used to determine the capacitance of arbitrarily shaped electrodes during sensor design.<ref name="Baxter" >{{Cite book
  |title=Capacitive Sensors: Design and Applications
  |author=Larry K. Baxter
  |publisher=John Wiley & Sons
  |year=1996
  |isbn=078035351X
  |chapter=Analytical solutions
  |url=http://books.google.co.uk/books?id=Tjd2laRnO4wC&pg=PA25&lpg=PA25&dq=teledeltos&source=bl&ots=NvX2nlzD_5&sig=jqIuhkVu61vtNa-3NPvyK-SufJ8&hl=en&sa=X&ei=v_PRT9OdCOOr0QWEnLmdBA&redir_esc=y#v=onepage&q=teledeltos&f=false
  |page=25
}}</ref>
 
== See also ==
* [[Finite element analysis]]
* [[Hydraulic analogy]]
 
== References ==
{{Reflist|group=note|liststyle=lower-roman}}
 
{{Reflist|colwidth=35em}}
 
[[Category:Analog computers]]
[[Category:Electrical engineering]]
[[Category:Sensors]]

Revision as of 22:29, 14 February 2014


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