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TSC2007IPW 数据表(PDF) 15 Page - Texas Instruments

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部件名 TSC2007IPW
功能描述  1.2V to 3.6V, 12-Bit, Nanopower, 4-Wire Micro TOUCH SCREEN CONTROLLER with I2C??Interface
PDF  41 Pages
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制造商  TI [Texas Instruments]
网页  http://www.ti.com
标志 TI - Texas Instruments

TSC2007IPW 数据表(HTML) 15 Page - Texas Instruments

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INTERNAL TEMPERATURE SENSOR
Converter
GND
V
DD
+IN
-IN
DV +
kT
q @ ln(N)
(3)
T +
q @ DV
k @ ln(N)
(4)
TSC2007
SBAS405 – MARCH 2007
OVERVIEW (continued)
In some applications, such as battery recharging, an ambient temperature measurement is required. The
temperature measurement technique used in the TSC2007 relies on the characteristics of a semiconductor
junction operating at a fixed current level. The forward diode voltage (VBE) has a well-defined characteristic
versus temperature. The ambient temperature can be predicted in applications by knowing the +25
°C value of
the VBE voltage and then monitoring the delta of that voltage as the temperature changes.
The TSC2007 offers two modes of temperature measurement. The first mode requires calibration at a known
temperature, but only requires a single reading to predict the ambient temperature. The TEMP1 diode, shown in
Figure 22, is used during this measurement cycle. This voltage is typically 580mV at +25
°C with a 10µA current.
The absolute value of this diode voltage can vary by a few millivolts; the temperature coefficient (TC) of this
voltage is very consistent at –2.1mV/
°C. During the final test of the end product, the diode voltage would be
stored at a known room temperature, in system memory, for calibration purposes by the user. The result is an
equivalent temperature measurement resolution of 0.35
°C/LSB (1LSB = 732µV with V
REF = 3.0V).
Figure 22. Functional Block Diagram of Temperature Measurement Mode
The second mode does not require a test temperature calibration, but uses a two-measurement (differential)
method to eliminate the need for absolute temperature calibration and for achieving 2
°C/LSB accuracy. This
mode requires a second conversion of the voltage across the TEMP2 diode with a resistance 80 times larger
than the TEMP1 diode. The voltage difference between the first (TEMP1) and second (TEMP2) conversion is
represented by:
Where:
N = the resistance ratio = 80.
k = Boltzmann's constant = 1.3807
× 10-23 J/K (joules/kelvins).
q = the electron charge = 1.6022
× 10-19 C (coulombs).
T = the temperature in kelvins (K).
This method can provide much improved absolute temperature measurement, but a lower resolution of
1.6
°C/LSB. The resulting equation to solve for T is:
Where:
∆V = V
BE (TEMP2) – VBE(TEMP1) (in mV)
∴ T = 2.648 ⋅ ∆V (in K)
or T = 2.648
⋅ ∆V – 273 (in °C)
Temperature 1 and temperature 2 measurements have the same timing as Figure 33 and Figure 34.
15
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