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产品型号QT118H-D的Datasheet PDF文件预览

lQ  
QProx™ QT118H  
OUCH  
C
HARGE-TRANSFER  
T
S
ENSOR  
Less expensive than many mechanical switches  
Projects a ‘touch button’ through any dielectric  
100% autocal for life - no adjustments required  
No active external components  
Vdd  
Out  
1
2
3
4
8
7
6
5
Vss  
Piezo sounder direct drive for ‘tactile’ click feedback  
LED drive for visual feedback  
2.5 ~ 5V single supply operation  
Sns2  
Sns1  
Gain  
10µA at 2.5V - very low power drain  
Opt1  
Opt2  
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  
APPLICATIONS -  
Light switches  
Industrial panels  
Appliance control  
Security systems  
Access systems  
Pointing devices  
Elevator buttons  
Toys & games  
The QT118H charge-transfer (“QT’”) touch sensor is a self-contained digital IC capable of detecting near-proximity or touch. It will  
project a sense field through almost any dielectric, like glass, plastic, stone, ceramic, and wood. It can also turn small metal-bearing  
objects into intrinsic sensors, making them respond to proximity or touch. This capability coupled with an ability to self calibrate  
continuously can lead to entirely new product concepts.  
The device is designed specifically for human interfaces, like control panels, appliances, toys, lighting controls, or anywhere a  
mechanical switch or button may be found; it may also be used for some material sensing and control applications provided that the  
presence duration of objects does not exceed the recalibration timeout interval.  
A piezo element can also be connected to create a feedback click sound.  
The IC requires only a common inexpensive capacitor in order to function. Average power consumption is under 20µA in most  
applications, allowing battery operation.  
The QT118H employs digital signal processing techniques pioneered by Quantum, designed to make it survive real-world  
challenges, such as ‘stuck sensor’ conditions and signal drift. Sensitivity is digitally determined for the highest possible stability. No  
external active components are required for operation.  
The device includes several user-selectable built in features. One, toggle mode, permits on/off touch control, for example for light  
switch replacement. Another makes the sensor output a pulse instead of a DC level, which allows the device to 'talk' over the power  
rail, permitting a simple 2-wire twisted-pair interface. Quantum’s unique HeartBeat™ signal is also included, allowing a host  
controller to continuously monitor the health of the device.  
By using the charge transfer principle, the IC delivers a level of performance clearly superior to older technologies in a highly  
cost-effective package.  
AVAILABLE OPTIONS  
TA  
00C to +700C  
-400C to +850C  
SOIC  
8-PIN DIP  
QT118H-DG  
-
-
QT118H-ISG  
lq  
©1999-2004 Quantum Research Group  
R1.08 / 0405  
Figure 1-1 Standard mode options  
1 - OVERVIEW  
The QT118H is a digital burst mode charge-transfer (QT)  
sensor designed specifically for touch controls; it includes all  
hardware and signal processing functions necessary to  
provide stable sensing under a wide variety of changing  
conditions. Only a few low cost, non-critical discrete external  
parts are required for operation.  
+2.5 ~ +5  
1
RE  
Vdd  
2
3
4
7
5
6
SENSING  
OUT  
SNS2  
GAIN  
SNS1  
Figure 1-1 shows the basic QT118H circuit using the device,  
with a conventional output drive and power supply  
connections. Figure 1-2 shows a second configuration using  
a common power/signal rail which can be a long twisted pair  
from a controller; this configuration uses the built-in pulse  
mode to transmit the output state to the host controller.  
ELECTRODE  
OPT1  
OPT2  
Rs  
Cs  
Cx  
2nF - 500nF  
Vss  
OUTPUT = DC  
TIMEOUT = 10 Secs  
TOGGLE = OFF  
GAIN = HIGH  
8
1.1 BASIC OPERATION  
The QT118H 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.  
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.  
The QT switches and charge measurement hardware  
functions are all internal to the QT118H (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.  
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).  
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).  
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.  
Piezo sounder drive: The QT118H 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 Cpiezo is in the proper range, no  
additional capacitor. If Cpiezo is too small, it can simply be  
‘topped up’ with a ceramic capacitor in parallel. The QT118H  
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.  
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.  
Figure 1-2 2-wire operation, self-powered  
+
3.5 - 5.5V  
10µF  
CMOS  
LOGIC  
1K  
Twisted  
pair  
1N4148  
1
Vdd  
SNS2  
RE  
2
3
4
7
SENSING  
ELECTRODE  
OUT  
n-ch Mosfet  
Cs  
5
6
OPT1 GAIN  
Rs  
Cx  
OPT2 SNS1  
Vss  
8
lq  
2
QT118H R1.08 / 0405  
1.3 ELECTRODE DESIGN  
Figure 1-3 Internal Switching & Timing  
ELECTRODE  
1.3.1 ELECTRODE  
G
EOMETRY AND  
S
IZE  
Result  
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  
QT118H 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.  
SNS2  
Cs  
Start  
Cx  
Done  
SNS1  
C harge  
Amp  
1.3.2 KIRCHOFF  
S  
CURRENT  
LAW  
Like all capacitance sensors, the  
QT118H relies on Kirchoffs Current  
Law (Figure 1-5) to detect the change  
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.  
in capacitance of the electrode. This law as applied to  
capacitive sensing requires that the sensors field current  
must complete a loop, returning back to its source in order for  
capacitance to be sensed. Although most designers relate to  
Kirchoffs 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  
Groundas 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 QT118H 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).  
picofarads back to local earth.  
1.3.3 VIRTUAL  
C
APACITIVE  
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 spacecapacitance 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 QT118H via earth. The QT118H's PCB  
however can be physically quite small, so there may be little  
free spacecoupling (Cx1 in Figure 1-4) between it and the  
environment to complete the return path. If the QT118H  
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.  
Figure 1-4 Kirchoff's Current Law  
C
X2  
Sense E lectrode  
A virtual capacitive groundcan be created by connecting the  
QT118Hs own circuit ground to:  
SENSOR  
- A nearby piece of metal or metallized housing;  
- A floating conductive ground plane;  
- Another electronic device (to which its might be  
connected already).  
C
X1  
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  
C
X3  
Surrounding environm ent  
lq  
3
QT118H R1.08 / 0405  
a slow rate, but only while there is no detection in effect. The  
rate of adjustment must be performed slowly, otherwise  
legitimate detections could be ignored. The QT118H drift  
compensates using a slew-rate limited change to the  
reference level; the threshold and hysteresis values are  
slaved to this reference.  
Table 1-1 Gain Strap Options  
Gain  
High  
Tie Pin 5 to:  
Leave open  
Pin 6  
Medium  
Low  
Pin 7  
Once an object is sensed, the drift compensation mechanism  
ceases since the signal is legitimately high, and therefore  
should not cause the reference level to change.  
1.3.5.2 Changing Cs, Cx  
The values of Cs and Cx have a dramatic effect on  
sensitivity, and Cs can be easily increased in value to  
improve gain. Sensitivity is directly proportional to Cs and  
inversely proportional to Cx:  
The QT118H's drift compensation is 'asymmetric': the  
reference level drift-compensates in one direction faster than  
it does in the other. Specifically, it compensates faster for  
decreasing signals than for increasing signals. Increasing  
signals should not be compensated for quickly, since an  
approaching finger could be compensated for partially or  
entirely before even touching the sense pad. However, an  
obstruction over the sense pad, for which the sensor has  
already made full allowance for, could suddenly be removed  
leaving the sensor with an artificially elevated reference level  
and thus become insensitive to touch. In this latter case, the  
sensor will compensate for the object's removal very quickly,  
usually in only a few seconds.  
k$CS  
S =  
Where kdepends on a variety of factors including the gain  
pin setting (see prior section), Vdd, etc.  
CX  
Sensitivity plots are shown in Figures 4-1 and 4-2, page 10.  
1.3.5.3 Electrode / Panel Adjustments  
Sensitivity can often be increased by using a bigger  
electrode, or reducing overlying panel thickness. Increasing  
electrode size can have a diminishing effect on gain, as the  
attendant higher values of Cx will start to reduce sensor gain.  
2.1.2 THRESHOLD AND  
H
YSTERESIS  
Also, 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.  
The internal signal threshold level can be set to one of three  
settings (Table 1-1). These are fixed with respect to the  
internal reference level, which in turn moves in accordance  
with the drift compensation mechanism.  
The panel or other intervening material can be made thinner,  
but again there are diminishing rewards for doing so. Panel  
material can also be changed to one having a higher  
dielectric constant, which will help propagate the field through  
to the front. Locally adding some conductive material to the  
panel (conductive materials essentially have an infinite  
dielectric constant) will also help; for example, adding carbon  
or metal fibers to a plastic panel will greatly increase frontal  
field strength, even if the fiber density is too low to make the  
plastic bulk-conductive.  
The QT118H employs a hysteresis dropout below the  
threshold level of 17% of the delta between the reference and  
threshold levels.  
2.1.3 MAX  
ON-DURATION  
If an object or material obstructs the sense pad the signal  
may rise enough to create a detection, preventing further  
operation. To prevent this, the sensor includes a timer which  
monitors detections. If a detection exceeds the timer setting,  
the timer causes the sensor to perform a full recalibration.  
This is known as the Max On-Duration feature.  
1.3.5.3 Ground Planes  
After the Max On-Duration interval, the sensor will once again  
function normally, even if partially or fully obstructed, to the  
best of its ability given electrode conditions. There are two  
timeout durations available via strap option: 10 and 60  
seconds.  
Grounds around and under the electrode and its SNS 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, and so  
ground areas around electrodes are discouraged. Keep  
ground, power, and other signals traces away from the  
electrodes and SNS wiring  
2.1.4 DETECTION  
INTEGRATOR  
It is desirable to suppress detections generated by electrical  
noise or from quick brushes with an object. To accomplish  
this, the QT118H incorporates a detect integration counter  
2 - QT118H SPECIFICS  
2.1 SIGNAL PROCESSING  
Figure 2-1 Drift Compensation  
The QT118H digitally processes all signals using  
a number of algorithms pioneered by Quantum.  
The algorithms are specifically designed to  
provide for high survivability in the face of all  
kinds of adverse environmental changes.  
Signal  
Hysteresis  
Threshold  
2.1.1 DRIFT  
COMPENSATION  
ALGORITHM  
Reference  
Signal drift can occur because of changes in Cx  
and Cs over time. It is crucial that drift be  
compensated for, otherwise false detections,  
non-detections, and sensitivity shifts will follow.  
Drift compensation (Figure 2-1) is performed by  
making the reference level track the raw signal at  
Output  
lq  
4
QT118H R1.08 / 0405  
that increments with each detection until a limit is reached,  
after which the output is activated. If no detection is sensed  
prior to the final count, the counter is reset immediately to  
zero. The required count is 4.  
Max On-Duration expires, whichever occurs first. If the latter  
occurs first, the sensor performs a full recalibration and the  
output becomes inactive until the next detection.  
In this mode, two nominal Max On-Duration timeouts are  
The Detection Integrator can also be viewed as a 'consensus' available: 10 and 60 seconds.  
filter, that requires four detections in four successive bursts to  
2.2.2 TOGGLE  
M
ODE  
O
UTPUT  
create an output. As the basic burst spacing is 95ms, if this  
spacing was maintained through 4 consecutive bursts the  
sensor would be very slow to respond. In the QT118H, after  
an initial detection is sensed, the remaining three bursts are  
spaced only about 2ms apart, so that the slowest reaction  
time possible is the fastest possible.  
This makes the sensor respond in an on/off mode like a flip  
flop. It is most useful for controlling power loads, for example  
in kitchen appliances, power tools, light switches, etc.  
Max On-Duration in Toggle mode is fixed at 10 seconds.  
When a timeout occurs, the sensor recalibrates but leaves  
the output state unchanged.  
2.1.5 FORCED  
S
ENSOR  
R
ECALIBRATION  
The QT118H has no recalibration pin; a forced recalibration  
is accomplished only when the device is powered up.  
However, the supply drain is so low it is a simple matter to  
treat the entire IC as a controllable load; simply driving the  
QT118H's Vdd pin directly from another logic gate or a  
microprocessor port (Figure 2-2) will serve as both power and  
'forced recal'. The source resistance of most CMOS gates  
and microprocessors is low enough to provide direct power  
without any problems. Almost any CMOS logic gate can  
directly power the QT118H.  
Table 2-1 Output Mode Strap Options  
Tie  
Pin 3 to:  
Tie  
Pin 4 to:  
Max On-  
Duration  
Vdd  
Vdd  
Gnd  
Gnd  
Vdd  
Gnd  
Gnd  
Vdd  
10s  
60s  
10s  
10s  
DC Out  
DC Out  
Toggle  
Pulse  
A 0.01uF minimum bypass capacitor close to the device is  
essential; without it the device can break into high frequency  
oscillation.  
2.2.3 PULSE  
M
ODE  
O
UTPUT  
This generates a positive pulse of 95ms duration with every  
new detection. It is most useful for 2-wire operation (see  
Figure 1-2), but can also be used when bussing together  
several devices onto a common output line with the help of  
steering diodes or logic gates, in order to control a common  
load from several places.  
Option strap configurations are read by the QT118H only on  
powerup. Configurations can only be changed by powering  
the QT118H down and back up again; a microcontroller can  
directly alter most of the configurations and cycle power to  
put them in effect.  
Max On-Duration is fixed at 10 seconds if in Pulse output  
mode.  
2.2 OUTPUT FEATURES  
The QT118H is designed for maximum flexibility and can  
accommodate most popular sensing requirements. These  
are selectable using strap options on pins OPT1 and OPT2.  
All options are shown in Table 2-1.  
The piezo beeper drive does not operate in Pulse mode.  
2.2.4 HEARTBEATOUTPUT  
The output has a full-time HeartBeat™ ‘healthindicator  
superimposed on it. This operates by taking 'Out' into a  
tri-state mode for 350µs once before every QT burst. This  
output state can be used to determine that the sensor is  
operating properly, or, it can be ignored using one of several  
simple methods.  
OPT1 and OPT2 should never be left floating. If they are  
floated, the device will draw excess power and the options  
will not be properly read on powerup. Intentionally, there are  
no pullup resistors on these lines, since pullup resistors add  
to power drain if the pin(s) are tied low.  
Since Out is normally low, a pullup resistor will create positive  
HeartBeat pulses (Figure 2-3) when the sensor is not  
detecting an object; when detecting an object, the output will  
remain active for the duration of the detection, and no  
HeartBeat pulse will be evident.  
2.2.1 DC MODE  
O
UTPUT  
The output of the device can respond in a DC mode, where  
the output is active-high upon detection. The output will  
remain active for the duration of the detection, or until the  
If the sensor is wired to a microcontroller as shown in Figure  
2-4, the controller can reconfigure the load resistor to either  
ground or Vcc depending on the output state of the device,  
so that the pulses are evident in either state.  
Figure 2-2 Powering From a CMOS Port Pin  
PORT X.m  
Electromechanical devices will usually ignore this short  
pulse. The pulse also has too low a duty cycle to visibly  
activate LEDs. It can be filtered completely if desired, by  
adding an RC timeconstant to filter the output, or if interfacing  
directly and only to a high-impedance CMOS input, by doing  
nothing or at most adding a small non-critical capacitor from  
Out to ground (Figure 2-5).  
0.01µF  
C MO S  
m ic rocontroller  
Vdd  
PORT X.n  
OUT  
QT118  
Vss  
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5
QT118H R1.08 / 0405  
Figure 2-3  
Getting HB pulses with a pullup resistor when not active  
Figure 2-4  
Using a micro to obtain HB pulses in either output state  
greatly reduced by placing a 470K resistor Rs in parallel with  
the resonator; this acts to slowly discharge the resonator,  
attenuating of the harmonic-rich audible step (Figure 2-6).  
2.2.5 PIEZO  
A
COUSTIC  
D
RIVE  
A piezo drive signal is generated for use with a piezo sounder  
immediately after a detection is made; the tone lasts for a  
nominal 95ms to create a tactile feedbacksound.  
Note that the piezo drive does not operate in Pulse mode.  
The sensor drives the piezo using an H-bridge configuration  
for the highest possible sound level. The piezo is connected  
across pins SNS1 and SNS2 in place of Cs or in addition to a  
parallel Cs capacitor. The piezo sounder should be selected  
to have a peak acoustic output in the 3.5kHz to 4.5kHz  
region.  
2.2.6 OUTPUT  
The QT118Hs output is active high and it can source or sink  
1mA of non-inductive current.  
D
RIVE  
Care should be taken when the IC and the load are both  
powered from the same supply, and the supply is minimally  
regulated. The device derives its internal references from the  
power supply, and sensitivity shifts can occur with changes in  
Vdd, as happens when loads are switched on. This can  
induce detection cycling, whereby an object is detected, the  
load is turned on, the supply sags, the detection is no longer  
sensed, the load is turned off, the supply rises and the object  
is reacquired, ad infinitum. To prevent this occurrence, the  
output should only be lightly loaded if the device is operated  
from an unregulated supply, e.g. batteries. Detection  
stiction, the opposite effect, can occur if a load is shed when  
Out is active.  
Since piezo sounders are merely high-K ceramic capacitors,  
the sounder will double as the Cs capacitor, and the piezo's  
metal disc can even act as the sensing electrode. Piezo  
transducer capacitances typically range from 6nF to 30nF in  
value; at the lower end of this range an additional capacitor  
should be added to bring the total Cs across SNS1 and  
SNS2 to at least 10nF, or possibly more if Cx is above 5pF.  
Piezo sounders have very high, uncharacterized thermal  
coefficients and should not be used if fast temperature  
swings are anticipated, especially at high gains. They are  
also generally unstable at high gains; even if the total value  
of Cs is largely from an added capacitor the piezo can cause  
periodic false detections.  
3 - CIRCUIT GUIDELINES  
The burst acquisition process induces a small but audible  
voltage step across the piezo resonator, which occurs when  
SNS1 and SNS2 rapidly discharge residual voltage stored on  
the resonator. The resulting slight clicking sound can be  
3.1 SAMPLE CAPACITOR  
When used for most applications, the charge sampler Cs can  
be virtually any plastic film or good quality ceramic capacitor.  
The type should be relatively stable in the anticipated  
Figure 2-5 Eliminating HB Pulses  
Figure 2-6 Piezo Sounder Circuit  
+2.5 ~ +5  
GATE OR  
MICRO INPUT  
1
RE  
Vdd  
2
3
4
7
5
6
SENSING  
2
3
4
7
5
6
OUT  
SNS1  
GAIN  
SNS2  
C M OS  
OUT  
SNS2  
GAIN  
SNS1  
ELECTRODE  
Co  
OPT1  
OPT2  
100pF  
Rs  
OPT1  
OPT2  
Cx  
Vss  
8
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6
QT118H R1.08 / 0405  
temperature range. If fast temperature swings are expected, Without this capacitor the part can break into high frequency  
especially with higher sensitivities, more stable capacitors be oscillation, get physically hot, stop working, or become  
required, for example PPS film. In most moderate gain  
applications (ie in most cases), low-cost X7R types will work  
fine.  
damaged.  
PCB Cleanliness: All capacitive sensors should be treated  
as highly sensitive circuits which can be influenced by stray  
conductive leakage paths. QT devices have a basic  
resolution in the femtofarad range; in this region, there is no  
such thing as no clean flux. Flux absorbs moisture and  
becomes conductive between solder joints, causing signal  
drift and resultant false detections or temporary loss of  
sensitivity. Conformal coatings can trap existing amounts of  
moisture which will then become highly temperature  
sensitive.  
3.2 ELECTRODE WIRING  
See also Section 3.4.  
The wiring of the electrode and its connecting trace is  
important to achieving high signal levels and low noise.  
Certain design rules should be adhered to for best results:  
1. Use a ground plane under the IC itself and Cs and Rs  
but NOT under Re, or under or closely around the  
electrode or its connecting trace. Keep ground away  
from these things to reduce stray loading (which will  
dramatically reduce sensitivity).  
The designer should strongly consider ultrasonic cleaning as  
part of the manufacturing process, and in more extreme  
cases, the use of conformal coatings after cleaning and  
baking.  
2. Keep Cs, Rs, and Re very close to the IC.  
3.3.1 SUPPLY  
CURRENT  
3. Make Re as large as possible. As a test, check to be  
sure that an increase of Re by 50% does not appreciably  
decrease sensitivity; if it does, reduce Re until the 50%  
test increase has a negligible effect on sensitivity.  
Measuring average power consumption is a challenging task  
due to the burst nature of the devices operation. Even a  
good quality RMS DMM will have difficulty tracking the  
relatively slow burst rate, and will show erratic readings.  
4. Do not route the sense wire near other livetraces  
containing repetitive switching signals; the trace will pick  
up noise from external signals.  
The easiest way to measure Idd is to put a very large  
capacitor, such as 2,700µF across the power pins, and put a  
220 ohm resistor from there back to the power source.  
Measure the voltage across the 220 resistor with a DMM and  
compute the current based on Ohms law. This circuit will  
average out current to provide a much smoother reading.  
3.3 POWER SUPPLY, PCB LAYOUT  
The power supply can range from 2.5 to 5.0 volts. At 2.5 volts  
current drain averages less than 10µA with Cs = 10nF,  
provided a 470K Rs resistor is used (Figure 1-1). Sample Idd  
curves are shown in Figure 4-3.  
To reduce the current consumption the most, use high or low  
gain pin settings only, the smallest value of Cs possible that  
works, and a 470K resistor (Rs) across Cs (Figure 1-1). Rs  
acts to help discharge capacitor Cs between bursts, and its  
presence substantially reduces power consumption.  
Higher values of Cs will raise current drain. Higher Cx values  
can actually decrease power drain. Operation can be from  
batteries, but be cautious about loads causing supply droop  
(see Output Drive, Section 2.2.6) if the batteries are  
unregulated.  
3.3.2 ESD PROTECTION  
In cases where the electrode is placed behind a dielectric  
panel, the IC will be protected from direct static discharge.  
However even with a panel transients can still flow into the  
electrode via induction, or in extreme cases via dielectric  
breakdown. Porous materials may allow a spark to tunnel  
right through the material. Testing is required to reveal any  
problems. The device has diode protection on its terminals  
which will absorb and protect the device from most ESD  
events; the usefulness of the internal clamping will depending  
on the dielectric properties, panel thickness, and rise time of  
the ESD transients.  
As battery voltage sags with use or fluctuates slowly with  
temperature, the IC will track and compensate for these  
changes automatically with only minor changes in sensitivity.  
If the power supply is shared with another electronic system,  
care should be taken to assure that the supply is free of  
digital spikes, sags, and surges which can adversely affect  
the device. The IC will track slow changes in Vdd, but it can  
be affected by rapid voltage steps.  
if desired, the supply can be regulated using a conventional  
low current regulator, for example CMOS LDO regulators that  
have nanoamp quiescent currents. Care should be taken that  
the regulator does not have a minimum load specification,  
which almost certainly will be violated by the QT118's low  
current requirement. Furthermore, some LDO regulators are  
unable to provide adequate transient regulation between the  
quiescent and acquire states, creating Vdd disturbances that  
will interfere with the acquisition process. This can usually be  
solved by adding a small extra load from Vdd to ground, such  
as 10K ohms, to provide a minimum load on the regulator.  
The best method available to suppress ESD and RFI is to  
insert a series resistor Re in series with the electrode as  
shown in Figure 1-1. The value should be the largest that  
does not affect sensing performance. If Re is too high, the  
gain of the sensor will decrease.  
Because the charge and transfer times of the QT118 are  
relatively long (~2µs), the circuit can tolerate a large value of  
Re, often more than 10k ohms in most cases.  
Diodes or semiconductor transient protection devices or  
MOV's on the electrode trace are not advised; these devices  
have extremely large amounts of nonlinear parasitic  
capacitance which will swamp the capacitance of the  
electrode and cause false detections and other forms of  
instability. Diodes also act as RF detectors and will cause  
serious RF immunity problems.  
Conventional non-LDO type regulators are usually more  
stable than slow, low power CMOS LDO types. Consult the  
regulator manufacturer for recommendations.  
For proper operation a 100nF (0.1uF) ceramic bypass  
capacitor must be used between Vdd and Vss; the bypass  
cap should be placed very close to the devices power pins.  
lq  
7
QT118H R1.08 / 0405  
In brief summary, the following design rules should be  
adhered to for best ESD and EMC results:  
3.4 EMC AND RELATED NOISE ISSUES  
External AC fields (EMI) due to RF transmitters or electrical  
noise sources can cause false detections or unexplained  
shifts in sensitivity.  
1. Use only SMT components.  
2. Keep Cs, Rs, Re and Vdd bypass cap close to the IC.  
The influence of external fields on the sensor is reduced by  
means of the Rseries described in Section 3.2. The Cs  
capacitor and Rseries (see Figure 1-1) form a natural  
low-pass filter for incoming RF signals; the roll-off frequency  
of this network is defined by -  
3. Maximize Re to the limit where sensitivity is not  
noticeably affected.  
4. Do not place the electrode or its connecting trace near  
other traces, or near a ground plane.  
1
5. Do use a ground plane under and around the QT118  
itself, back to the regulator and power connector (but not  
beyond the Cs capacitor).  
FR =  
2RseriesCs  
If for example Cs = 22nF, and Rseries = 10K ohms, the rolloff  
frequency to EMI is 723Hz, vastly lower than any credible  
external noise source (except for mains frequencies i.e. 50 /  
60 Hz). However, Rseries and Cs must both be placed very  
close to the body of the IC so that the lead lengths between  
them and the IC do not form an unfiltered antenna at very  
high frequencies.  
6. Do not place an electrode (or its wiring) of one QT  
device near the electrode or wiring of another device, to  
prevent cross interference.  
7. Keep the electrode (and its wiring) away from other  
traces carrying AC or switched signals.  
8. If there are LEDs or LED wiring near the electrode or its  
wiring (ie for backlighting of the key), bypass the LED  
wiring to ground on both its ends.  
PCB layout, grounding, and the structure of the input circuitry  
have a great bearing on the success of a design to withstand  
electromagnetic fields and be relatively noise-free.  
9. Use a voltage regulator just for the QT118 to eliminate  
power noise coupling from other switching sources.  
Make sure the regulators transient load stability provides  
for stable voltage just before each burst commences.  
For further tips on construction, PCB design, and EMC issues  
browse the application notes and faq at www.qprox.com  
lq  
8
QT118H R1.08 / 0405  
4.1 ABSOLUTE MAXIMUM SPECIFICATIONS  
Operating temp. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . as designated by suffix  
Storage temp. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -55OC to +125OC  
V
DD. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -0.5 to +6.5V  
Max continuous pin current, any control or drive pin. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20mA  
Short circuit duration to ground, any pin. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . infinite  
Short circuit duration to VDD, any pin. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . infinite  
Voltage forced onto any pin. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -0.6V to (Vdd + 0.6) Volts  
4.2 RECOMMENDED OPERATING CONDITIONS  
V
DD. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . +2.5 to 5.0V  
Short-term supply ripple+noise. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5mV  
Long-term supply stability. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 100mV  
Cs value. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10nF to 500nF  
Cx value. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0 to 100pF  
Rs value. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 470K  
4.3 AC SPECIFICATIONS  
Vdd = 3.0, Cs = 10nF, Rs = 470K, Cx = 10pF, Gain = High, Ta = 20OC, unless otherwise noted.  
Parameter  
Description  
Min  
Typ  
Max  
Units  
Notes  
T
RC  
Recalibration time  
550  
2
ms  
µs  
T
Q
Charge, transfer duration  
Burst spacing interval  
T
BS  
75  
95  
ms  
ms  
@ 5.0V Vdd  
@ 3.3V Vdd  
T
BL  
Burst length  
0.5  
3.6  
50  
ms  
ms  
kHz  
ms  
ms  
µs  
Depends on Cs, Cx  
T
R
P
Response time  
129  
4
F
Piezo drive frequency  
Piezo drive duration  
Pulse output width on Out  
Heartbeat pulse width  
Burst frequency  
4.4  
T
P
75  
T
PO  
HB  
75  
T
300  
165  
F
Q
kHz  
4.4 SIGNAL PROCESSING  
Vdd = 3.0, Cs = 10nF, Rs = 470K, Cx = 10pF, Gain = High, Ta = 20OC, unless otherwise noted.  
Description  
Min  
Typ  
Max  
Units  
Notes  
Threshold differential  
6, 12, or 24  
counts  
%
1
2
Hysteresis  
17  
4
Detect integrator filter length  
Positive drift compensation rate  
Negative drift compensation rate  
Post-detection recalibration timer duration (typical min/max)  
samples  
ms/level  
ms/level  
secs  
750  
75  
4
4
10  
60  
3, 4  
Note 1: Pin options  
Note 2: Percentage of signal threshold  
Note 3: Pin option  
Note 4: Cs, Cx dependent  
lq  
9
QT118H R1.08 / 0405  
4.5 DC SPECIFICATIONS  
Vdd = 3.0, Cs = 10nF, Rs = 470K, Cx = 10pF, Gain = High, Ta = 20OC Unless otherwise noted.  
Parameter  
Description  
Min  
Typ  
Max  
Units  
Notes  
VDDL  
VDDL  
IDD  
Guaranteed min Vdd  
Guaranteed min Vdd  
Supply current  
2.45  
2.95  
V
V
-I suffix  
-E suffix  
30  
10  
8
µA  
@ Vdd = 5.0V  
@ Vdd = 3.3V  
@ Vdd = 2.5V  
V
DDS  
Supply turn-on slope  
Low input logic level  
High input logic level  
Low output voltage  
High output voltage  
Input leakage current  
Acquisition resolution  
Sensitivity range  
100  
2.2  
V/s  
V
Required for proper startup  
OPT1, OPT2  
V
IL  
0.8  
0.6  
V
HL  
V
OPT1, OPT2  
V
OL  
V
OUT, 4mA sink  
OUT, 1mA source  
OPT1, OPT2  
V
OH  
IL  
Vdd-0.7  
V
I
1
14  
28  
µA  
bits  
fF  
A
R
9
S
1,000  
Note 2  
Figure 4-1 - Typical Threshold Sensitivity vs. Cx,  
High Gain, at Selected Values of Cs; Vdd = 3.0  
Figure 4-2 - Typical Threshold Sensitivity vs. Cx,  
Medium Gain, Selected Values of Cs; Vdd = 3.0  
10.00  
1.00  
0.10  
0.01  
10.00  
1.00  
0.10  
0.01  
10nF  
10nF  
20nF  
20nF  
50nF  
50nF  
100nF  
200nF  
500nF  
100nF  
200nF  
500nF  
0
10  
20  
30  
40  
0
10  
20  
30  
40  
Cx Load, pF  
Cx Load, pF  
Figure 4-3 Typical Supply Current Vs Vdd  
Rs = 470K, Cx = 10pF, Gain = High  
40  
35  
30  
25  
20  
15  
10  
5
Cs = 20nF  
..  
Cs = 10nF  
2.5  
3
3.5  
4
4.5  
5
Vdd  
lq  
10  
QT118H R1.08 / 0405  
4.6 MECHANICAL  
Package type: 8pin Dual-In-Line  
Millimeters  
Inches  
Max  
SYMBOL  
Min  
Max  
Notes  
Min  
Notes  
a
A
6.096  
7.62  
7.112  
8.255  
10.922  
7.62  
-
0.24  
0.3  
0.28  
0.325  
0.43  
0.3  
M
m
Q
P
9.017  
7.62  
Typical  
BSC  
0.355  
0.3  
Typical  
BSC  
0.889  
0.254  
0.355  
1.397  
2.489  
3.048  
0.381  
3.048  
-
0.035  
0.01  
0.014  
0.055  
0.098  
0.12  
0.015  
0.12  
-
-
-
-
L
0.559  
1.651  
2.591  
3.81  
-
0.022  
0.065  
0.102  
0.15  
-
L1  
F
Typical  
Typical  
R
r
S
3.556  
4.064  
7.062  
9.906  
0.381  
0.14  
0.16  
0.3  
S1  
Aa  
x
7.62  
BSC  
0.3  
BSC  
8.128  
0.203  
0.32  
0.008  
0.39  
0.015  
Y
Package type: 8pin SOIC  
Millimeters  
Inches  
Max  
SYMBOL  
Min  
Max  
Notes  
Min  
Notes  
M
W
Aa  
H
h
4.800  
5.816  
3.81  
4.979  
6.198  
3.988  
1.728  
0.762  
1.27  
0.189  
0.229  
0.15  
0.196  
0.244  
0.157  
0.068  
0.01  
0.05  
0.019  
0.04  
0.01  
0.03  
8º  
1.371  
0.101  
1.27  
0.054  
0.004  
0.050  
0.014  
0.02  
D
L
BSC  
BSC  
0.355  
0.508  
0.19  
0.483  
1.016  
0.249  
0.762  
8º  
E
e
0.007  
0.229  
0º  
ß
0.381  
0º  
Ø
5 - ORDERING INFORMATION  
PART  
TEMP RANGE  
PACKAGE  
MARKING  
PDIP  
Pb-Free  
SO-8  
QT118H-D  
0 - 70C  
QT118H-G  
QT1 + T + G  
or QT118H-IG  
QT118H-ISG  
-40 - 85C  
Pb-Free  
lq  
11  
QT118H R1.08 / 0405  
6 - SOIC MARKING DIAGRAMS  
VERSION ‘A’  
Lot code  
(last letter varies)  
©QT1 T F  
Lot Code  
0214HB6.G  
QPROX C  
'G' ending  
indicates Pb-free  
package  
Pin 1 Dimple  
VERSION ‘B’  
'G' ending  
indicates Pb-free  
package  
QT118H-IG  
0214HB6C  
©QPROX  
Lot Code  
Pin 1 Dimple  
lq  
12  
QT118H R1.08 / 0405  
NOTES  
lq  
13  
QT118H R1.08 / 0405  
lQ  
Copyright © 1999 - 2004 QRG Ltd. All rights reserved.  
Patented and patents pending  
Corporate Headquarters  
1 Mitchell Point  
Ensign Way, Hamble SO31 4RF  
Great Britain  
Tel: +44 (0)23 8056 5600 Fax: +44 (0)23 80565600  
admin@qprox.com  
www.qprox.com  
North America  
651 Holiday Drive Bldg. 5 / 300  
Pittsburgh, PA 15220 USA  
Tel: 412-391-7367 Fax: 412-291-1015  
This device covered under one or more of the following United States and international patents: 5,730,165, 6,288,707, 6,377,009, 6,452,514,  
6,457,355, 6,466,036, 6,535,200. Numerous further patents are pending which may apply to this device or the applications thereof.  
The specifications set out in this document are subject to change without notice. All products sold and services supplied by QRG are subject  
to our Terms and Conditions of sale and supply of services which are available online at www.qprox.com and are supplied with every order  
acknowledgement. QProx, QTouch, QMatrix, QLevel, and QSlide are trademarks of QRG. QRG products are not suitable for medical  
(including lifesaving equipment), safety or mission critical applications or other similar purposes. Except as expressly set out in QRG's Terms  
and Conditions, no licenses to patents or other intellectual property of QRG (express or implied) are granted by QRG in connection with the  
sale of QRG products or provision of QRG services. QRG will not be liable for customer product design and customers are entirely  
responsible for their products and applications which incorporate QRG's products.  
配单直通车
QT118H-D产品参数
型号:QT118H-D
生命周期:Transferred
IHS 制造商:ATMEL CORP
零件包装代码:DIP
包装说明:DIP,
针数:8
Reach Compliance Code:unknown
HTS代码:8542.39.00.01
风险等级:5.57
模拟集成电路 - 其他类型:ANALOG CIRCUIT
JESD-30 代码:R-PDIP-T8
长度:9.9695 mm
功能数量:1
端子数量:8
最高工作温度:70 °C
最低工作温度:
封装主体材料:PLASTIC/EPOXY
封装代码:DIP
封装形状:RECTANGULAR
封装形式:IN-LINE
座面最大高度:4.064 mm
最大供电电压 (Vsup):5.5 V
最小供电电压 (Vsup):2.5 V
标称供电电压 (Vsup):5 V
表面贴装:NO
温度等级:COMMERCIAL
端子形式:THROUGH-HOLE
端子节距:2.54 mm
端子位置:DUAL
宽度:7.62 mm
Base Number Matches:1
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