1.3.2 8-pin UDFN/USON
Figure 1-2. Basic Circuit Configuration
Cs
OUT
VDD
SNSK
SNS
SYNC/MODE
VSS
4
6
8
1
5
7
Vdd
Rs
Cx
SENSE
ELECTRODE
Note: A bypass capacitor should be tightly wired
between Vdd and Vss and kept close to pin 5.
2
3
NC
NC
AT42QT1010
© 2017 Microchip Technology Inc.
Datasheet
DS40001946A-page 7
2. Overview of the AT42QT1010
2.1 Introduction
The AT42QT1010 is a digital burst mode charge-transfer sensor that is capable of detecting near-
proximity or touch, making it ideal for implementing touch controls.
With the proper electrode and circuit design, the self-contained digital IC will project a touch or proximity
field to several centimeters through any dielectric like glass, plastic, stone, ceramic, and even most kinds
of wood. It can also turn small metal-bearing objects into intrinsic sensors, making them responsive to
proximity or touch. This capability, coupled with its ability to self-calibrate, can lead to entirely new product
concepts.
The QT1010 is designed specifically for human interfaces like control panels, appliances, toys, lighting
controls, or anywhere a mechanical switch or button may be found. It includes all hardware and signal
processing functions necessary to provide stable sensing under a wide variety of changing conditions.
Only a single low-cost capacitor is required for operation.
2.2 Basic Operation
Figure 1-1 and Figure 1-2 show basic circuits.
The QT1010 employs bursts of charge-transfer cycles to acquire its signal. Burst mode permits power
consumption in the microamp range, dramatically reduces RF emissions, lowers susceptibility to EMI, and
yet permits excellent response time. Internally the signals are digitally processed to reject impulse noise,
using a “consensus” filter which requires four consecutive confirmations of a detection before the output
is activated.
The QT switches and charge measurement hardware functions are all internal to the QT1010.
2.3 Electrode Drive
For optimum noise immunity, the electrode should only be connected to SNSK.
In all cases, the rule Cs >> Cx must be observed for proper operation; a typical load capacitance (Cx)
ranges from 5–20 pF while Cs is usually about 2–50 nF.
Increasing amounts of Cx destroy gain; therefore, it is important to limit the amount of stray capacitance
on both SNS terminals. This can be done, for example, by minimizing trace lengths and widths, and
keeping these traces away from power or ground traces or copper pours.
The traces and any components associated with SNS and SNSK will become touch sensitive and should
be treated with caution to limit the touch area to the desired location.
A series resistor, Rs, should be placed in line with SNSK to the electrode to suppress ESD and EMC
effects.
2.4 Sensitivity
2.4.1 Introduction
The sensitivity on the QT1010 is a function of things like the value of Cs, electrode size and capacitance,
electrode shape and orientation, the composition and aspect of the object to be sensed, the thickness
AT42QT1010
© 2017 Microchip Technology Inc.
Datasheet
DS40001946A-page 8
and composition of any overlaying panel material, and the degree of ground coupling of both sensor and
object.
2.4.2 Increasing Sensitivity
In some cases it may be desirable to increase sensitivity; for example, when using the sensor with very
thick panels having a low dielectric constant, or when the device is used as a proximity sensor. Sensitivity
can often be increased by using a larger electrode or reducing panel thickness. Increasing electrode size
can have diminishing returns, since high values of Cx will reduce sensor gain.
The value of Cs also has a dramatic effect on sensitivity, and this can be increased in value with the
trade-off of slower response time and more power. Increasing the electrode's surface area will not
substantially increase touch sensitivity if its diameter is already much larger in surface area than the
object being detected. Panel material can also be changed to one having a higher dielectric constant,
which will better help to propagate the field.
In the case of proximity detection, usually the object being detected is on an approaching hand, so a
larger surface area can be effective.
Ground planes around and under the electrode and its SNSK trace will cause high Cx loading and
destroy gain. The possible signal-to-noise ratio benefits of ground area are more than negated by the
decreased gain from the circuit so ground areas around electrodes are discouraged. Metal areas near the
electrode will reduce the field strength and increase Cx loading and should be avoided, if possible. Keep
ground away from the electrodes and traces.
2.4.3 Decreasing Sensitivity
In some cases the QT1010 may be too sensitive. In this case gain can be easily lowered further by
decreasing Cs.
2.4.4 Proximity Sensing
By increasing the sensitivity, the QT1010 can be used as a very effective proximity sensor, allowing the
presence of a nearby object (typically a hand) to be detected.
In this scenario, as the object being sensed is typically a hand, very large electrode sizes can be used,
which is extremely effective in increasing the sensitivity of the detector. In this case, the value of Cs will
also need to be increased to ensure improved sensitivity, as mentioned in Section 2.4.2. Note that,
although this affects the responsiveness of the sensor, it is less of an issue in proximity sensing
applications; in such applications it is necessary to detect simply the presence of a large object, rather
than a small, precise touch.
AT42QT1010
© 2017 Microchip Technology Inc.
Datasheet
DS40001946A-page 9

AT42QT1010-MAHR

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IC SENSR TOUCH/PROX 1CH 8-UDFN
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