The QT118HA is a Flash version of the QT118H. The QT118HA is form, fit and function
compatible with the older device, except that the QT118HA is more sensitive than the
older device, necessitating a significant reduction in Cs capacitance. See Section 1 on page 2 for
differences.
This device is intended as a replacement for the QT118H in existing
designs already in production, but is not recommended for new designs.
For further device migration plans please
consult your local Atmel or Quantum representative.
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QT118HA_AR1.02_0408
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Q QT118HA-ISG
NOT RECOMMENDED FOR NEW DESIGNS
Sns2
Vss
Sns1
GainOpt2
Opt1
Out
Vdd 1
2
3
4 5
6
7
8
QT118HA
Less expensive than many mechanical switches
Projects a ‘touch button’ through any dielectric
100% autocal for life - no adjustments required
No active external components
Piezo sounder direct drive for ‘tactile’ click feedback
LED drive for visual feedback
2 ~ 5V single supply operation
10µ
µµ
µA at 2.5V - very low power drain
Toggle mode for on/off control (via option pins)
10s or 60s auto-recalibration timeout (via option pins)
Pulse output mode (via option pins)
Gain settings in 3 discrete levels
Simple 2-wire operation possible
HeartBeat™ health indicator on output
Pb-Free package
1 - OVERVIEW
The QT118HA is intended to replace the QT118H as a lower
cost alternative. This device functions identically to the QT118H,
except that it is more sensitive. To compensate for the sensitivity
increase, it is required to do either of these two things:
1. Increase the Cx loading to ground on SNS2 by 10pF
2. Decrease the Cs value
Option 1 is very simple and guarantees that the sensitivity of the
QT118HA is identical to the older device. Option 2 requires
some trial and error to test the sensitivity of the touch pad or
prox field, so that it is about the same as before. Cs changes
ranging from 10 - 60% may be required depending on the circuit
layout and electrode design.
All other aspects of this datasheet are identical to the QT118H
datasheet except for this section and specifications on pages 9
and 10, and the part marking.
1.1 BASIC OPERATION
The QT118HA employs short, low duty cycle bursts of QT cycles
to acquire capacitance. Burst mode permits power consumption
in the low 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 QT118HA (Figure 1-3). A single-slope
switched capacitor ADC includes both the required QT charge
and transfer switches in a configuration that provides direct ADC
conversion. The sensitivity depends on the values of Cs, Cx,
and to a smaller degree, Vdd. Vdd is used as the charge
reference voltage.
Higher values of Cs increase gain; higher values of Cx load
reduce it. The value of Cs can thus be increased to allow larger
values of Cx to be tolerated (Figures 4-1 and 4-2, page 10).
Piezo sounder drive: The QT118HA can drive a piezo sounder
after a detection for feedback. The piezo sounder replaces or
augments the Cs capacitor; this works since piezo sounders are
also capacitors, albeit with a large thermal drift coefficient. If
C
piezo
is in the proper range, no additional capacitor. If C
piezo
is
too small, it can simply be ‘topped up’ with a ceramic capacitor
in parallel. The QT118HA drives a ~4kHz signal across SNS1
and SNS2 to make the piezo (if installed) sound a short tone for
75ms immediately after detection, to act as an audible
confirmation.
Option pins allow the selection or alteration of several special
features and sensitivity.
1.2 ELECTRODE DRIVE
The internal ADC treats Cs as a floating transfer capacitor; as a
direct result, the sense electrode can in theory be connected to
either SNS1 or SNS2 with no performance difference. However,
the noise immunity of the device is improved by connecting the
electrode to SNS2, preferably via a series resistor Re (Figure
1-1) to roll off higher harmonic frequencies, both outbound and
inbound.
In order to reduce power consumption and to assist in
discharging Cs between acquisition bursts, a 470K series
resistor Rs should always be connected across Cs (Figure 1-1).
The rule Cs >> Cx must be observed for proper operation.
Normally Cx is on the order of 10pF or so, while Cs might be
10nF (10,000pF), or a ratio of about 1:1000.
It is important to minimize the amount of unnecessary stray
capacitance Cx, for example by minimizing trace lengths and
widths and backing off adjacent ground traces and planes so as
keep gain high for a given value of Cs, and to allow for a larger
sensing electrode size if so desired.
The PCB traces, wiring, and any components associated with or
in contact with SNS1 and SNS2 will become touch sensitive and
should be treated with caution to limit the touch area to the
desired location.
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q 2 QT118HA_AR1.02_0408
Figure 1-1 Standard mode options
SENSING
ELECTRODE
Cs
Rs
2nF - 500nF
3
4 6
5
1
+2.5 ~ +5
72
OUT
OPT1
OPT2
GAIN
SNS1
SNS2
Vss
Vdd
OUTPUT = DC
TIMEOUT = 10 Secs
TOGGLE = OFF
GAIN = HIGH
C
x
8
R
E
+2 ~ +5
Figure 1-2 2-wire operation, self-powered
+
10µF
1N4148
n-ch Mosfet
CMOS
LOGIC
3.5 - 5.5V
1K Twisted
pair
C
s
8
OUT
OPT1
OPT2
GAIN
SNS1
SNS2
Vss
Vdd
3
4 6
5
1
72
R
s
SENSING
ELECTRODE
C
x
R
E
1.3 ELECTRODE DESIGN
1.3.1 ELECTRODE GEOMETRY AND SIZE
There is no restriction on the shape of
the electrode; in most cases common
sense and a little experimentation can
result in a good electrode design. The
QT118HA will operate equally well with
long, thin electrodes as with round or
square ones; even random shapes are
acceptable. The electrode can also be
a 3-dimensional surface or object.
Sensitivity is related to electrode
surface area, orientation with respect
to the object being sensed, object
composition, and the ground coupling
quality of both the sensor circuit and
the sensed object.
1.3.2 KIRCHOFFS CURRENT LAW
Like all capacitance sensors, the
QT118HA relies on Kirchoff’s Current
Law (Figure 1-5) to detect the change
in capacitance of the electrode. This law as applied to
capacitive sensing requires that the sensor’s field current
must complete a loop, returning back to its source in order for
capacitance to be sensed. Although most designers relate to
Kirchoff’s law with regard to hardwired circuits, it applies
equally to capacitive field flows. By implication it requires that
the signal ground and the target object must both be coupled
together in some manner for a capacitive sensor to operate
properly. Note that there is no need to provide actual
hardwired ground connections; capacitive coupling to ground
(Cx1) is always sufficient, even if the coupling might seem
very tenuous. For example, powering the sensor via an
isolated transformer will provide ample ground coupling,
since there is capacitance between the windings and/or the
transformer core, and from the power wiring itself directly to
'local earth'. Even when battery powered, just the physical
size of the PCB and the object into which the electronics is
embedded will generally be enough to couple a few
picofarads back to local earth.
1.3.3 VIRTUAL CAPACITIVE GROUNDS
When detecting human contact (e.g. a fingertip), grounding
of the person is never required. The human body naturally
has several hundred picofarads of ‘free space’ capacitance to
the local environment (Cx3 in Figure 1-4), which is more than
two orders of magnitude greater than that required to create
a return path to the QT118HA via earth. The QT118HA's PCB
however can be physically quite small, so there may be little
‘free space’ coupling (Cx1 in Figure 1-4) between it and the
environment to complete the return path. If the QT118HA
circuit ground cannot be earth grounded by wire, for example
via the supply connections, then a ‘virtual capacitive ground’
may be required to increase return coupling.
A ‘virtual capacitive ground’ can be created by connecting the
QT118HA’s own circuit ground to:
- A nearby piece of metal or metallized housing;
- A floating conductive ground plane;
- Another electronic device (to which its might be
connected already).
Free-floating ground planes such as metal foils should
maximize exposed surface area in a flat plane if possible. A
square of metal foil will have little effect if it is rolled up or
crumpled into a ball. Virtual ground planes are more effective
and can be made smaller if they are physically bonded to
other surfaces, for example a wall or floor.
‘Ground’ as applied to capacitive fields can also mean power
wiring or signal lines. The capacitive sensor, being an AC
device, needs only an AC ground return.
1.3.5 SENSITIVITY ADJUSTMENT
1.3.5.1 Gain Pin
The QT118HA can be set for one of 3 gain levels using
option pin 5 (Table 1-1). This sensitivity change is made by
altering the internal numerical threshold level required for a
detection. Note that sensitivity is also a function of other
things: like the values of Cs and Cx, electrode size, shape,
and orientation, the composition and aspect of the object to
be sensed, the thickness and composition of any overlaying
panel material, and the degree of ground coupling of both
sensor and object.
The Gain input should never be connected to a pullup or
pulldown resistor or tied to anything other than SNS1 or
SNS2, or left unconnected (for high gain setting).
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Figure 1-3 Internal Switching & Timing
C
s
C
x
SNS2
SNS1
ELECTRODE
Single -Slo pe 14-bit
Switched Cap acitor ADC
Charg e
Am p
Burst C ontroller
Result
Do ne
Start
Figure 1-4 Kirchoff's Current Law
Sense E lectrode
C
X2
Su rro und ing e n viro nm en t
C
X3
SENSO R
C
X1

QT118HA-ISG

Mfr. #:
Manufacturer:
Microchip Technology / Atmel
Description:
Interface - Specialized Qtouch IC
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
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