Affecting Mutual Capacitance w/ an External Field

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The discussion focuses on the mechanics of projected capacitive touchscreens, particularly the iPhone's design, which features a grid of capacitors formed by layers of conductors and a dielectric layer. The main inquiry is whether it's possible to influence the mutual capacitance of these capacitors from a distance using an external electric field. While it is suggested that an external field could be detected by the conductor matrix, achieving sufficient focus for resolution is challenging. An alternative approach mentioned involves using a different dielectric material and a laser pointer to affect capacitance at specific points. The conversation highlights the complexity of the touchscreen's operation, including its ability to filter out electromagnetic interference and register touch based on larger changes in the grid.
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I've been playing around with projected capacitive touchscreens - specifically, the iPhone's. I've attached a white paper that outlines the details, but the basic idea is as follows:
An iPhone's touchscreen has a dielectric layer sandwiched between a layer of conductors arranged in rows and a layer of conductors arranged in columns. The result is a grid of capacitors that can be independently driven. When a finger (or anything capable of sapping enough charge) comes close enough to these pseudo-capacitors, the field between them is altered, and a touch is registered. ("Close enough" has been tuned to exactly the point at which a finger touches the iPhone's glass screen.)

What I'm wondering is - is it possible to alter these fields in the same way, but from further away than originally intended? Perhaps with a generated E-field? In general, can you alter the mutual capacitance of two conductors with an external field?

Thanks in advance!
 
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pin0ut said:
I've been playing around with projected capacitive touchscreens - specifically, the iPhone's. I've attached a white paper that outlines the details, but the basic idea is as follows:
An iPhone's touchscreen has a dielectric layer sandwiched between a layer of conductors arranged in rows and a layer of conductors arranged in columns. The result is a grid of capacitors that can be independently driven. When a finger (or anything capable of sapping enough charge) comes close enough to these pseudo-capacitors, the field between them is altered, and a touch is registered. ("Close enough" has been tuned to exactly the point at which a finger touches the iPhone's glass screen.)

What I'm wondering is - is it possible to alter these fields in the same way, but from further away than originally intended? Perhaps with a generated E-field? In general, can you alter the mutual capacitance of two conductors with an external field?

Thanks in advance!

Welcome to the PF.

You could pick up an external field with the conductor matrix, but it would be hard to make the external field focused enough to give good resolution.

You might be able to use an alternate dielectric material between the row and column electrodes, and use a laser pointer to alter the capacitance at the laser spot...
 
Thanks!

Resolution isn't actually a huge issue. The goal isn't to alter the field in a single pseudo-capacitor in the grid, but rather several of them. The iPhone's touchscreen controller has to deal with EMI and false positive touches, so it basically scans for "blobs" or small regions of change on the grid. If the blob is large enough and the changes large enough, a touch is registered in the rough center of the blob. All this is done in hardware, and is probably a close-guarded secret, so the specifics are hard to come by.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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