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AD22105ARZ-REEL PDF预览

AD22105ARZ-REEL

更新时间: 2024-01-25 13:50:53
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亚德诺 - ADI 开关
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AD22105ARZ-REEL 数据手册

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AD22105  
OUTPUT SECTION  
Response of the AD22105 internal die temperature to abrupt  
changes in ambient temperatures can be modeled by a single  
time constant exponential function. Figure 11 shows typical  
response plots for moving and still air. The time constant, τ  
(time to reach 63.2% of the final value), is dependent on θJA and  
the thermal capacities of the chip and the package. Table I lists  
the effective τ for moving and still air. Copper printed circuit  
board connections were neglected in the analysis; however, they  
will sink or conduct heat directly through the AD22105’s solder  
plated copper leads. When faster response is required, a therm-  
ally conductive grease or glue between the AD22105 and the  
surface temperature being measured should be used.  
The output of the AD22105 is the collector of an NPN transistor.  
When the ambient temperature of the device exceeds the  
programmed setpoint temperature, this transistor is activated  
causing its collector to become a low impedance. A pull-up  
resistor, such as the internal 200 kprovided, is needed to  
observe a change in the output voltage. For versatility, the  
optional pull-up resistor has not been permanently connected  
to the output pin. Instead, this resistor is undedicated and  
connects from Pin 7 (VS) to Pin 1 (RPULL-UP). In order to use  
RPULL-UP a single connection should be made from Pin 1  
(RPULL-UP) to Pin 2 (OUT).  
The 200 kpull-up resistor can drive CMOS loads since  
essentially no static current is required at these inputs. When  
driving “LS” and other bipolar family logic inputs a parallel  
resistor may be necessary to supply the 20 µA–50 µA IIH (High  
Level Input Current) specified for such devices. To determine  
the current required, the appropriate manufacturer’s data sheet  
should be consulted. When the output is switched, indicating an  
over temperature condition, the output is capable of pulling  
down with 10 mA at a voltage of about 375 mV. This allows for  
a fan out of 2 with standard bipolar logic and 20 with “LS”  
family logic.  
Table I. Thermal Resistance (SO-8)  
Medium  
JA (؇C/Watt)  
(sec)*  
Moving Air**  
100  
3.5  
Without Heat Sink  
Still Air  
190  
15  
Without Heat Sink  
NOTES  
**The time constant is defined as the time to reach 63.2% of the final tempera-  
ture change.  
Low power indicator LEDs (up to 10 mA) can be driven  
directly from the output pin of the AD22105. In most cases a  
small series resistor (usually of several hundred ohms) will be  
required to limit the current to the LED and the output  
transistor of the AD22105.  
**1200 CFM.  
USING THE AD22105 AS A COOLING SETPOINT  
DETECTOR  
The AD22105 can be used to detect transitions from higher  
temperatures to lower temperatures by programming the  
setpoint temperature 4°C greater than the desired trip point  
temperature. The 4°C is necessary to compensate for the  
nominal hysteresis value designed into the device. A more  
precise value of the hysteresis can be obtained from Figure 6. In  
this mode, the logic state of the output will indicate a HIGH for  
under temperature conditions. The total device error will be  
slightly greater than the specification value due to uncertainty in  
hysteresis.  
MOUNTING CONSIDERATIONS  
If the AD22105 is thermally attached and properly protected, it  
can be used in any measuring situation where the maximum  
range of temperatures encountered is between –40°C and  
+150°C. Because plastic IC packaging technology is employed,  
excessive mechanical stress must be avoided when fastening the  
device with a clamp or screw-on heat tab. Thermally conductive  
epoxy or glue is recommended for typical mounting conditions.  
In wet or corrosive environments, an electrically isolated metal  
or ceramic well should be used to protect the AD22105.  
APPLICATION HINTS  
EMI Suppression  
THERMAL ENVIRONMENT EFFECTS  
Noisy environments may couple electromagnetic energy into the  
RSET node causing the AD22105 to falsely trip or untrip. Noise  
sources, which typically come from fast rising edges, can be  
coupled into the device capacitively. Furthermore, if the output  
signal is brought close the RSET pin, energy can couple from the  
OUT pin to the RSET pin potentially causing oscillation. Stray  
capacitance can come from several places such as, IC sockets,  
multiconductor cables, and printed circuit board traces. In some  
cases, it can be corrected by constructing a Faraday shield  
around the RSET pin, for example, by using a shielded cable with  
the shield grounded. However, for best performance, cables  
should be avoided and the AD22105 should be soldered directly  
to a printed circuit board whenever possible. Figure 13 shows a  
sample printed circuit board layout with low inter-pin capaci-  
tance and Faraday shielding. If stray capacitance is unavoidable,  
and interference or oscillation occurs, a low impedance capaci-  
tor should be connected from the RSET pin to the GND pin.  
This capacitor must be considerably larger than the estimated  
stray capacitance. Typically several hundred picofarads will cor-  
rect the problem.  
The thermal environment in which the AD22105 is used  
determines two performance traits: the effect of self-heating on  
accuracy and the response time of the sensor to rapid changes in  
temperature. In the first case, a rise in the IC junction tempera-  
ture above the ambient temperature is a function of two variables:  
the power consumption of the AD22105 and the thermal  
resistance between the chip and the ambient environment, θJA.  
Self-heating error can be derived by multiplying the power  
dissipation by θJA. Because errors of this type can vary widely for  
surroundings with different heat sinking capacities, it is  
necessary to specify θJA under several conditions. Table I shows  
how the magnitude of self-heating error varies relative to the  
environment. A typical part will dissipate about 230 µW at  
room temperature with a 3.3 V supply and negligible output  
loading. In still air, without a “heat sink,” Table I indicates a  
θJA of 190°C/W, which yields a temperature rise of 0.04°C.  
Thermal rise of the die will be considerably less in an environ-  
ment of turbulent or constant moving air or if the device is in  
direct physical contact with a solid (or liquid) body.  
REV. 0  
–7–  

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