Cp3bt26 – National CP3BT26 User Manual

Page 82

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82

CP3BT26

16.2.2

Measuring Pen Force

Figure 27 shows equivalent circuits for the driver modes
used to measure the X, Y, and Z coordinates, in which Z rep-
resents pen force. In this discussion, the ohmic resistance
of the drivers is neglected (see Section 16.2.3), and series
resistance between the node of interest and the ADC is ig-
nored because it has no significant effect.

Figure 27.

Touchscreen Driver Modes

In the following examples, the ADC is assumed to operate
in single-ended mode to produce conversion values be-
tween 0 and 2047, however the same principles could be
extended to differential mode to recover the full range of the
ADC.

In Sample X mode, the X plate is driven between VCC and
ground, so that a value measured at node A on the TSY+ or
TSY- inputs is the center tap of a resistor-divider network.
The end-to-end resistance RXP of the X plate is:

The value measured at node A is proportional to the ratio
between the resistance to ground and the resistance of the
X plate:

Solving for RX2, the resistance is:

Similarly, in Sample Y mode the value measured at node B
on the TSX+ or TSX- inputs is proportional to the ratio be-
tween the resistance to ground and the resistance RYP of
the Y plate:

Because end-to-end resistance RYP of the Y plate is:

The previous equation can be rewritten as:

Solving for RY1, the resistance is:

Now that the resistance values RX2 and RY1 are known, it
is possible to calculate the value of the plate-to-plate con-
tact resistance, RZ, given the value measured at node C on
the TSX+ input in Sample Z mode. Node C is a tap in a re-
sistor-divider network composed of three resistors, such
that:

Solving for RZ, the resistance is:

The resistance RZ is proportional to the force of pen con-
tact.

16.2.3

Compensation for Driver Resistance

Plate resistances between opposite electrodes range from
100 ohms to 1k ohm. Because of the 6-ohm driver resis-
tance, some significant voltage drop will be experienced be-
tween, for example, TSX- and AGND. A 200-ohm plate will
drop:

With a 2.5V supply, this is 70 mV. A 12-bit ADC has 4096
possible values, so each value covers a range of 610 µV at
2.5V. A voltage drop of 70 mV across each of the low-ohmic
drivers reduces the number of available ADC values by:

This effective loss of resolution can be handled in a number
of ways.

1. The voltages on, for example, TSY+ and TSY- can be

sampled before sampling TSX+ and TSX-. Then, scal-
ing can be applied in software to convert the samples
to the full (4096-bit) range. This technique will not re-
cover any resolution, however it is worthy of some con-
sideration because touchscreen data is typically
passed to two applications:
Signature Analysis—only the raw data is required. No
absolute positioning is necessary.
Screen Overlay—for example, for cursor positioning.
In this application, a scaling or calibration is performed
to correctly overlay the touchscreen coordinates onto
the display. Because of this calibration, it is not even
necessary to sample TSY+ and TSY-.

2. The ADC has a positive voltage reference input which

can be internally connected to the TSY+ terminal. This
means that the number of available ADC values is in-
creased to:

Software scaling could be applied to this value if re-
quired (as with technique 1, above), but no additional
resolution is achieved.

DS188

VCC

RX1

RX2

A

Sample X

TOUCH_CFG = 001

VCC

RY1

RY2

B

Sample Y

TOUCH_CFG = 010

RZ

RX2

C

VCC

RY1

Sample Z

TOUCH_CFG = 100

RXP

RX1

RX2

+

=

A

2047

-------------

RX2

RXP

-------------

=

RX2

RXP

A

2047

-------------

×

=

B

2047

-------------

RY2

RYP

-------------

=

RYP

RY1

RY2

+

=

B

2047

-------------

RYP

RY1

RYP

-------------------------------

=

RY1

RYP

1

B

2047

-------------

×

=

C

2047

-------------

RX2

RY1

RZ

RX2

+

+

----------------------------------------------

=

RZ

RX2

2047

C

C

-----------------------

×

RY1

=

6

200

6

6

+

+

-----------------------------

AVCC

AGND

(

)

×

70 mV

2

×

610 uV

--------------------------

230

=

4096

70 mV

610 uV

--------------------

3981

=

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