Datasheet LT1962EMS8-5, LT1962EMS8-3, LT1962EMS8-2.5, LT1962EMS8 Datasheet (Linear Technology)

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LT1962 Series
300mA, Low Noise,
Micropower
LDO Regulators
April 2000
Low Noise: 20µV
(10Hz to 100kHz)
Output Current: 300mA
Low Quiescent Current: 30µA
Wide Input Voltage Range: 1.8V to 20V
Low Dropout Voltage: 270mV
Very Low Shutdown Current: < 1µA
No Protection Diodes Needed
Fixed Output Voltages: 2.5V, 3V, 3.3V, 5V
Adjustable Output from 1.22V to 20V
Stable with 3.3µF Output Capacitor
Stable with Aluminum, Tantalum or Ceramic Capacitors
Reverse Battery Protection
No Reverse Current
Overcurrent and Overtemperature Protected
8-Lead MSOP Package
The LT®1962 series are micropower, low noise, low dropout regulators. The devices are capable of supplying 300mA of output current with a dropout voltage of 300mV. Designed for use in battery-powered systems, the low 30µA quiescent current makes them an ideal choice. Quiescent current is well controlled; it does not rise in dropout as it does with many other regulators.
A key feature of the LT1962 regulators is low output noise. With the addition of an external 0.01µF bypass capacitor, output noise drops to 20µV
RMS
over a 10Hz to 100kHz
bandwidth. The LT1962 regulators are stable with output capacitors as low as 3.3µF. Small ceramic capacitors can be used without the series resistance required by other regulators.
Internal protection circuitry includes reverse battery pro­tection, current limiting, thermal limiting and reverse current protection. The parts come in fixed output volt­ages of 2.5V, 3V, 3.3V and 5V, and as an adjustable device with a 1.22V reference voltage. The LT1962 regulators are available in the 8-lead MSOP package.
3.3V Low Noise Regulator
Cellular Phones
Battery-Powered Systems
Noise-Sensitive Instrumentation Systems
, LTC and LT are registered trademarks of Linear Technology Corporation.
IN
SHDN
0.01µF
10µF
1962 TA01
OUT
SENSE
V
IN
3.7V TO 20V
BYP
GND
LT1962-3.3
3.3V AT 300mA 20µV
RMS
NOISE
1µF
+
DESCRIPTIO
U
FEATURES
APPLICATIO S
U
TYPICAL APPLICATIO
U
Final Electrical Specifications
LOAD CURRENT (mA)
0
DROPOUT VOLTAGE (mV)
400
350
300
250
200
150
100
50
0
1962 TA02
100
200
30050
150
250
Dropout Voltage
Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen­tation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
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LT1962 Series
(Note 1)
IN Pin Voltage........................................................ ±20V
OUT Pin Voltage .................................................... ±20V
Input to Output Differential Voltage (Note 2) ......... ±20V
SENSE Pin Voltage ............................................... ±20V
ADJ Pin Voltage ...................................................... ±7V
BYP Pin Voltage....................................................±0.6V
SHDN Pin Voltage................................................. ±20V
Output Short-Circut Duration.......................... Indefinite
Operating Junction Temperature Range
(Note 3) ............................................ –40°C to 125°C
Storage Temperature Range ................. –65°C to 150°C
Lead Temperature (Soldering, 10 sec)..................300°C
Consult factory for Industrial and Military grade parts.
PARAMETER CONDITIONS MIN TYP MAX UNITS
Minimum Operating Voltage I
LOAD
= 300mA 1.8 2.3 V
Regulated Output Voltage LT1962-2.5 VIN = 3V, I
LOAD
= 1mA 2.475 2.500 2.525 V
(Note 5) 3.5V < V
IN
< 20V, 1mA < I
LOAD
< 300mA 2.435 2.500 2.565 V
LT1962-3 VIN = 3.5V, I
LOAD
= 1mA 2.970 3.000 3.030 V
4V < V
IN
< 20V, 1mA < I
LOAD
< 300mA 2.925 3.000 3.075 V
LT1962-3.3 VIN = 3.8V, I
LOAD
= 1mA 3.267 3.300 3.333 V
4.3V < V
IN
< 20V, 1mA < I
LOAD
< 300mA 3.220 3.300 3.380 V
LT1962-5 VIN = 5.5V, I
LOAD
= 1mA 4.950 5.000 5.050 V
6V < V
IN
< 20V, 1mA < I
LOAD
< 300mA 4.875 5.000 5.125 V
ADJ Pin Voltage LT1962 VIN = 2V, I
LOAD
= 1mA 1.208 1.220 1.232 V
(Notes 4, 5) 2.3V < V
IN
< 20V, 1mA < I
LOAD
< 300mA 1.190 1.220 1.250 V
Line Regulation LT1962-2.5 ∆VIN = 3V to 20V, I
LOAD
= 1mA 15 mV
LT1962-3 ∆V
IN
= 3.5V to 20V, I
LOAD
= 1mA 15 mV
LT1962-3.3 ∆V
IN
= 3.8V to 20V, I
LOAD
= 1mA 15 mV
LT1962-5 ∆V
IN
= 5.5V to 20V, I
LOAD
= 1mA 15 mV
LT1962 (Note 4) ∆V
IN
= 2V to 20V, I
LOAD
= 1mA 15 mV
Load Regulation LT1962-2.5 VIN = 3.5V, ∆I
LOAD
= 1mA to 300mA 5 12 mV
V
IN
= 3.5V, ∆I
LOAD
= 1mA to 300mA 25 mV
LT1962-3 VIN = 4V, ∆I
LOAD
= 1mA to 300mA 7 15 mV
V
IN
= 4V, ∆I
LOAD
= 1mA to 300mA 30 mV
LT1962-3.3 VIN = 4.3V, ∆I
LOAD
= 1mA to 300mA 7 17 mV
V
IN
= 4.3V, ∆I
LOAD
= 1mA to 300mA 33 mV
LT1962-5 VIN = 6V, ∆I
LOAD
= 1mA to 300mA 12 25 mV
V
IN
= 6V, ∆I
LOAD
= 1mA to 300mA 50 mV
LT1962 (Note 4) VIN = 2.3V, ∆I
LOAD
= 1mA to 300mA 2 6 mV
V
IN
= 2.3V, ∆I
LOAD
= 1mA to 300mA 12 mV
The denotes specifications which apply over the full operating temperature range, otherwise specifications are TA = 25°C. (Note 3)
ORDER PART
NUMBER
LT1962EMS8 LT1962EMS8-2.5 LT1962EMS8-3 LT1962EMS8-3.3 LT1962EMS8-5
MS8 PART MARKING
LTML LTPT LTPQ LTPS LTPR
T
JMAX
= 150°C, θJA = 125°C/W
SEE THE APPLICATIONS INFORMATION SECTION
FOR ADDITIONAL
INFORMATION ON
THERMAL RESISTANCE
*PIN 2: SENSE FOR LT1962-2.5/LT1962-3/ LT1962-3.3/LT1962-5. ADJ FOR LT1962
1 2 3 4
OUT
SENSE/ADJ*
BYP
GND
8 7 6 5
IN NC NC SHDN
TOP VIEW
MS8 PACKAGE
8-LEAD PLASTIC MSOP
ELECTRICAL CHARACTERISTICS
PACKAGE/ORDER I FOR ATIO
UU
W
ABSOLUTE AXI U RATI GS
WWWU
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LT1962 Series
Dropout Voltage I
LOAD
= 10mA 0.10 0.15 V
V
IN
= V
OUT(NOMINAL)
I
LOAD
= 10mA 0.21 V
(Notes 6, 7)
I
LOAD
= 50mA 0.15 0.20 V
I
LOAD
= 50mA 0.28 V
I
LOAD
= 100mA 0.18 0.24 V
I
LOAD
= 100mA 0.33 V
I
LOAD
= 300mA 0.27 0.33 V
I
LOAD
= 300mA 0.43 V
GND Pin Current I
LOAD
= 0mA 30 75 µA
V
IN
= V
OUT(NOMINAL)
I
LOAD
= 1mA 65 120 µA
(Notes 6, 8)
I
LOAD
= 50mA 1.1 1.6 mA
I
LOAD
= 100mA 23 mA
I
LOAD
= 300mA 812 mA
Output Voltage Noise C
OUT
= 10µF, C
BYP
= 0.01µF, I
LOAD
= 300mA, BW = 10Hz to 100kHz 20 µV
RMS
ADJ Pin Bias Current (Notes 4, 9) 30 100 nA Shutdown Threshold V
OUT
= Off to On 0.8 2 V
V
OUT
= On to Off 0.25 0.65 V
SHDN Pin Current V
SHDN
= 0V 0.01 0.5 µA
(Note 10) V
SHDN
= 20V 1 5 µA
Quiescent Current in Shutdown VIN = 6V, V
SHDN
= 0V 0.1 1 µA
Ripple Rejection VIN – V
OUT
= 1.5V (Avg), V
RIPPLE
= 0.5V
P-P
, f
RIPPLE
= 120Hz, 55 65 dB
I
LOAD
= 300mA
Current Limit VIN = 7V, V
OUT
= 0V 700 mA
V
IN
= V
OUT(NOMINAL)
+ 1V, V
OUT
= –0.1V 320 mA
Input Reverse Leakage Current VIN = –20V, V
OUT
= 0V 1mA
Reverse Output Current LT1962-2.5 V
OUT
= 2.5V, VIN < 2.5V 10 20 µA
(Note 11) LT1962-3 V
OUT
= 3V, VIN < 3V 10 20 µA
LT1962-3.3 V
OUT
= 3.3V, VIN < 3.3V 10 20 µA
LT1962-5 V
OUT
= 5V, VIN < 5V 10 20 µA
LT1962 (Note 4) V
OUT
= 1.22V, VIN < 1.22V 5 10 µA
PARAMETER CONDITIONS MIN TYP MAX UNITS
The denotes specifications which apply over the full operating temperature range, otherwise specifications are TA = 25°C. (Note 2)
Note 6: To satisfy requirements for minimum input voltage, the LT1962
(adjustable version) is tested and specified for these conditions with an external resistor divider (two 250k resistors) for an output voltage of
2.44V. The external resistor divider will add a 5µA DC load on the output. Note 7: Dropout voltage is the minimum input to output voltage differential
needed to maintain regulation at a specified output current. In dropout, the output voltage will be equal to: VIN – V
DROPOUT
.
Note 8: GND pin current is tested with VIN = V
OUT(NOMINAL)
and a current source load. This means the device is tested while operating in its dropout region. This is the worst-case GND pin current. The GND pin current will decrease slightly at higher input voltages.
Note 9: ADJ pin bias current flows into the ADJ pin. Note 10: SHDN pin current flows into the SHDN pin. This current is
included in the specification for GND pin current. Note 11: Reverse output current is tested with the IN pin grounded and the
OUT pin forced to the rated output voltage. This current flows into the OUT pin and out the GND pin.
Note 1: Absolute Maximum Ratings are those values beyond which the life of a device may be impaired.
Note 2: Absolute maximum input to output differential voltage can not be achieved with all combinations of rated IN pin and OUT pin voltages. With the IN pin at 20V, the OUT pin may not be pulled below 0V. The total measured voltage from in to out can not exceed ±20V.
Note 3: The LT1962 regulators are tested and specified under pulse load conditions such that T
J
TA. The LT1962 is 100% tested at TA = 25°C.
Performance at –40°C and 125°C is assured by design, characterization and correlation with statistical process controls.
Note 4: The LT1962 (adjustable version) is tested and specified for these conditions with the ADJ pin connected to the OUT pin.
Note 5: Operating conditions are limited by maximum junction temperature. The regulated output voltage specification will not apply for all possible combinations of input voltage and output current. When operating at maximum input voltage, the output current range must be limited. When operating at maximum output current, the input voltage range must be limited.
ELECTRICAL CHARACTERISTICS
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LT1962 Series
reducing output voltage noise to a typical 20µV
RMS
over a 10Hz to 100kHz bandwidth. If not used, this pin must be left unconnected.
GND (Pin 4): Ground. SHDN (Pin 5): Shutdown. The SHDN pin is used to put the
LT1962 regulators into a low power shutdown state. The output will be off when the SHDN pin is pulled low. The SHDN pin can be driven either by 5V logic or open­collector logic with a pull-up resistor. The pull-up resistor is required to supply the pull-up current of the open­collector gate, normally several microamperes, and the SHDN pin current, typically 1µA. If unused, the SHDN pin must be connected to VIN. The device will not function if the SHDN pin is not connected.
NC (Pins 6, 7): No Connect. For best thermal perfor­mance, these pins are not internally connected. For im­proved power handling capabilities, these pins can be connected to the PC board.
IN (Pin 8): Input. Power is supplied to the device through the IN pin. A bypass capacitor is required on this pin if the device is more than six inches away from the main input filter capacitor. In general, the output impedance of a battery rises with frequency, so it is advisable to include a bypass capacitor in battery-powered circuits. A bypass capacitor in the range of 1µF to 10µF is sufficient. The LT1962 regulators are designed to withstand reverse voltages on the IN pin with respect to ground and the OUT pin. In the case of a reverse input, which can happen if a battery is plugged in backwards, the device will act as if there is a diode in series with its input. There will be no reverse current flow into the regulator and no reverse voltage will appear at the load. The device will protect both itself and the load.
OUT (Pin 1): Output. The output supplies power to the load. A minimum output capacitor of 3.3µF is required to prevent oscillations. Larger output capacitors will be required for applications with large transient loads to limit peak voltage transients. See the Applications Information section for more information on output capacitance and reverse output characteristics.
SENSE (Pin 2): Sense. For fixed voltage versions of the LT1962 (LT1962-2.5/LT1962-3/LT1962-3.3/LT1962-5), the SENSE pin is the input to the error amplifier. Optimum regulation will be obtained at the point where the SENSE pin is connected to the OUT pin of the regulator. In critical applications, small voltage drops are caused by the resis­tance (RP) of PC traces between the regulator and the load. These may be eliminated by connecting the SENSE pin to the output at the load as shown in Figure 1 (Kelvin Sense Connection). Note that the voltage drop across the exter­nal PC traces will add to the dropout voltage of the regulator. The SENSE pin bias current is 10µA at the nominal rated output voltage. The SENSE pin can be pulled below ground (as in a dual supply system where the regulator load is returned to a negative supply) and still allow the device to start and operate.
ADJ (Pin 2): Adjust. For the adjustable LT1962, this is the input to the error amplifier. This pin is internally clamped to ±7V. It has a bias current of 30nA which flows into the pin. The ADJ pin voltage is 1.22V referenced to ground and the output voltage range is 1.22V to 20V.
BYP (Pin 3): Bypass. The BYP pin is used to bypass the reference of the LT1962 to achieve low noise performance from the regulator. The BYP pin is clamped internally to ±0.6V (one VBE). A small capacitor from the output to this pin will bypass the reference to lower the output voltage noise. A maximum value of 0.01µF can be used for
Figure 1. Kelvin Sense Connection
IN
SHDN
1962 F01
R
P
OUT
V
IN
SENSE
GND
LT1962
R
P
4
2
1
5
8
+
+
LOAD
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LT1962 Series
The LT1962 series are 300mA low dropout regulators with micropower quiescent current and shutdown. The devices are capable of supplying 300mA at a dropout voltage of 300mV. Output voltage noise can be lowered to 20µV
RMS
over a 10Hz to 100kHz bandwidth with the addition of a
0.01µF reference bypass capacitor. Additionally, the refer- ence bypass capacitor will improve transient response of the regulator, lowering the settling time for transient load conditions. The low operating quiescent current (30µA) drops to less than 1µA in shutdown. In addition to the low quiescent current, the LT1962 regulators incorporate sev­eral protection features which make them ideal for use in battery-powered systems. The devices are protected against both reverse input and reverse output voltages. In battery backup applications where the output can be held up by a backup battery when the input is pulled to ground, the LT1962-X acts like it has a diode in series with its output and prevents reverse current flow. Additionally, in dual supply applications where the regulator load is re­turned to a negative supply, the output can be pulled below ground by as much as 20V and still allow the device to start and operate.
Adjustable Operation
The adjustable version of the LT1962 has an output voltage range of 1.22V to 20V. The output voltage is set by the ratio of two external resistors as shown in Figure 2. The device servos the output to maintain the ADJ pin voltage at 1.22V referenced to ground. The current in R1 is then equal to 1.22V/R1 and the current in R2 is the current in R1 plus the ADJ pin bias current. The ADJ pin bias current, 30nA at 25°C, flows through R2 into the ADJ pin. The
Figure 2. Adjustable Operation
output voltage can be calculated using the formula in Figure 2. The value of R1 should be no greater than 250k to minimize errors in the output voltage caused by the ADJ pin bias current. Note that in shutdown the output is turned off and the divider current will be zero.
The adjustable device is tested and specified with the ADJ pin tied to the OUT pin for an output voltage of 1.22V. Specifications for output voltages greater than 1.22V will be proportional to the ratio of the desired output voltage to
1.22V: V
OUT
/1.22V. For example, load regulation for an output current change of 1mA to 300mA is –2mV typical at V
OUT
= 1.22V. At V
OUT
= 12V, load regulation is:
(12V/1.22V)(–2mV) = –19.7mV
Bypass Capacitance and Low Noise Performance
The LT1962 regulators may be used with the addition of a bypass capacitor from V
OUT
to the BYP pin to lower output voltage noise. A good quality low leakage capacitor is recommended. This capacitor will bypass the reference of the regulator, providing a low frequency noise pole. The noise pole provided by this bypass capacitor will lower the output voltage noise to as low as 20µV
RMS
with the
addition of a 0.01µF bypass capacitor. Using a bypass capacitor has the added benefit of improving transient response. With no bypass capacitor and a 10µF output capacitor, a 10mA to 300mA load step will settle to within 1% of its final value in less than 100µs. With the addition of a 0.01µF bypass capacitor, the output will settle to within 1% for a 10mA to 300mA load step in less than 10µs, with total output voltage deviation of less than 2.5%. However, regulator start-up time is inversely proportional to the size of the bypass capacitor, slowing to 15ms with a 0.01µF bypass capacitor and 10µF output capacitor.
Output Capacitance and Transient Response
The LT1962 regulators are designed to be stable with a wide range of output capacitors. The ESR of the output capacitor affects stability, most notably with small capaci­tors. A minimum output capacitor of 3.3µF with an ESR of 3 or less is recommended to prevent oscillations. The LT1962-X is a micropower device and output transient response will be a function of output capacitance. Larger values of output capacitance decrease the peak deviations
IN
1962 F02
R2
OUT
V
IN
V
OUT
ADJ
GND
LT1962
R1
+
VV
R R
IR
VV InA
OUT ADJ
ADJ
ADJ
=+
 
 
+
()()
=
122 1
2 1
2
122
30
.
.
AT 25 C
OUTPUT RANGE = 1.22V TO 20V
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LT1962 Series
and provide improved transient response for larger load current changes. Bypass capacitors, used to decouple individual components powered by the LT1962, will in­crease the effective output capacitor value. With larger capacitors used to bypass the reference (for low noise operation), larger values of output capacitance are needed. For 100pF of bypass capacitance, 4.7µF of output capaci- tor is recommended. With a 1000pF bypass capacitor or larger, a 6.8µF output capacitor is recommended.
Extra consideration must be given to the use of ceramic capacitors. Ceramic capacitors are manufactured with a variety of dielectrics, each with different behavior across temperature and applied voltage. The most common dielectrics used are Z5U, Y5V, X5R and X7R. The Z5U and Y5V dielectrics are good for providing high capacitance in a small package, but exhibit strong voltage and tempera­ture coefficients as shown in Figures 3 and 4. When used with a 5V regulator, a 10µF Y5V capacitor can exhibit an effective value as low as 1µF to 2µF over the operating temperature range. The X5R and X7R dielectrics result in more stable characteristics and are more suitable for use as the output capacitor. The X7R type has better stability across temperature, while the X5R is less expensive and is available in higher values.
Voltage and temperature coefficients are not the only sources of problems. Some ceramic capacitors have a piezoelectric response. A piezoelectric device generates voltage across its terminals due to mechanical stress,
Figure 4. Ceramic Capacitor Temperature Characteristics
Figure 3. Ceramic Capacitor DC Bias Characteristics
DC BIAS VOLTAGE (V)
CHANGE IN VALUE (%)
1962 F04
20
0
–20
–40
–60
–80
–100
0
4
8
10
26
12
14
X5R
Y5V
16
BOTH CAPACITORS ARE 16V, 1210 CASE SIZE, 10µF
TEMPERATURE (°C)
–50
40
20
0
–20
–40
–60
–80
–100
25 75
1962 F04
–25 0
50 100 125
Y5V
CHANGE IN VALUE (%)
X5R
BOTH CAPACITORS ARE 16V, 1210 CASE SIZE, 10µF
similar to the way a piezoelectric accelerometer or micro­phone works. For a ceramic capacitor the stress can be induced by vibrations in the system or thermal transients. The resulting voltages produced can cause appreciable amounts of noise, especially when a ceramic capacitor is used for noise bypassing. A ceramic capacitor produced Figure 5’s trace in response to light tapping from a pencil. Similar vibration induced behavior can masquerade as increased output voltage noise.
Figure 5. Noise Resulting from Tapping on a Ceramic Capacitor
LT1962-5 C
OUT
= 10µF
C
BYP
= 0.01µf
I
LOAD
= 100mA
V
OUT
500µV/DIV
100ms/DIV
1962 F05
Thermal Considerations
The power handling capability of the device will be limited by the maximum rated junction temperature (125°C). The power dissipated by the device will be made up of two components:
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LT1962 Series
The power dissipated by the device will be equal to:
I
OUT(MAX)(VIN(MAX)
– V
OUT
) + I
GND(VIN(MAX)
)
where,
I
OUT(MAX)
= 100mA
V
IN(MAX)
= 6V
I
GND
at (I
OUT
= 100mA, VIN = 6V) = 2mA
So,
P = 100mA(6V – 3.3V) + 2mA(6V) = 0.28W
The thermal resistance will be in the range of 110°C/W to 140°C/W depending on the copper area. So the junction temperature rise above ambient will be approximately equal to:
0.28W(125°C/W) = 35.3°C
The maximum junction temperature will then be equal to the maximum junction temperature rise above ambient plus the maximum ambient temperature or:
T
JMAX
= 50°C + 35.3°C = 85.3°C
Protection Features
The LT1962 regulators incorporate several protection features which make them ideal for use in battery-powered circuits. In addition to the normal protection features associated with monolithic regulators, such as current limiting and thermal limiting, the devices are protected against reverse input voltages, reverse output voltages and reverse voltages from output to input.
Current limit protection and thermal overload protection are intended to protect the device against current overload conditions at the output of the device. For normal opera­tion, the junction temperature should not exceed 125°C.
The input of the device will withstand reverse voltages of 20V. Current flow into the device will be limited to less than 1mA (typically less than 100µA) and no negative voltage will appear at the output. The device will protect both itself and the load. This provides protection against batteries which can be plugged in backward.
The output of the LT1962 can be pulled below ground without damaging the device. If the input is left open circuit or grounded, the output can be pulled below ground by 20V. For fixed voltage versions, the output will act like a large resistor, typically 500k or higher, limiting current
1. Output current multiplied by the input/output voltage differential: (I
OUT
)(VIN – V
OUT
), and
2. GND pin current multiplied by the input voltage: (I
GND
)(VIN).
The GND pin current can be estimated using specification in the Electrical Characteristics table. Power dissipation will be equal to the sum of the two components listed above.
The LT1962 series regulators have internal thermal limit­ing designed to protect the device during overload condi­tions. For continuous normal conditions, the maximum junction temperature rating of 125°C must not be exceeded. It is important to give careful consideration to all sources of thermal resistance from junction to ambient. Additional heat sources mounted nearby must also be considered.
For surface mount devices, heat sinking is accomplished by using the heat spreading capabilities of the PC board and its copper traces. Copper board stiffeners and plated through-holes can also be used to spread the heat gener­ated by power devices.
The following table lists thermal resistance for several different board sizes and copper areas. All measurements were taken in still air on 1/16" FR-4 board with one ounce copper.
Table 1. Measured Thermal Resistance
COPPER AREA THERMAL RESISTANCE
TOPSIDE* BACKSIDE BOARD AREA (JUNCTION-TO-AMBIENT)
2500mm22500mm
2
2500mm
2
110°C/W
1000mm22500mm
2
2500mm
2
115°C/W
225mm22500mm
2
2500mm
2
120°C/W
100mm22500mm
2
2500mm
2
130°C/W
50mm22500mm
2
2500mm
2
140°C/W
*Device is mounted on topside.
Calculating Junction Temperature
Example: Given an output voltage of 3.3V, an input voltage range of 4V to 6V, an output current range of 0mA to 100mA and a maximum ambient temperature of 50°C, what will the maximum junction temperature be?
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LT1962 Series
flow to less than 40µA. For adjustable versions, the output will act like an open circuit; no current will flow out of the pin. If the input is powered by a voltage source, the output will source the short-circuit current of the device and will protect itself by thermal limiting. In this case, grounding the SHDN pin will turn off the device and stop the output from sourcing the short-circuit current.
The ADJ pin of the adjustable device can be pulled above or below ground by as much as 7V without damaging the device. If the input is left open circuit or grounded, the ADJ pin will act like an open circuit when pulled below ground and like a large resistor (typically 100k) in series with a diode when pulled above ground.
In situations where the ADJ pin is connected to a resistor divider that would pull the ADJ pin above its 7V clamp voltage if the output is pulled high, the ADJ pin input current must be limited to less than 5mA. For example, a resistor divider is used to provide a regulated 1.5V output from the 1.22V reference when the output is forced to 20V. The top resistor of the resistor divider must be chosen to limit the current into the ADJ pin to less than 5mA when the ADJ pin is at 7V. The 13V difference between OUT and ADJ pin divided by the 5mA maximum current into the ADJ pin yields a minimum top resistor value of 2.6k.
In circuits where a backup battery is required, several different input/output conditions can occur. The output
voltage may be held up while the input is either pulled to ground, pulled to some intermediate voltage or is left open circuit. Current flow back into the output will follow the curve shown in Figure 6.
When the IN pin of the LT1962 is forced below the OUT pin or the OUT pin is pulled above the IN pin, input current will typically drop to less than 2µA. This can happen if the input of the device is connected to a discharged (low voltage) battery and the output is held up by either a backup battery or a second regulator circuit. The state of the SHDN pin will have no effect on the reverse output current when the output is pulled above the input.
Figure 6. Reverse Output Current
1962i LT/TP 0400 4K • PRINTED IN USA
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RELATED PARTS
PART NUMBER DESCRIPTION COMMENTS
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APPLICATIO S I FOR ATIO
WUUU
OUTPUT VOLTAGE (V)
01
REVERSE OUTPUT CURRENT (µA)
30
40
50
60
70
80
90
100
897
1962 F06
20 10
0
23
465
10
LT1962
LT1962-2.5
LT1962-3
LT1962-3.3
LT1962-5
TJ = 25°C V
IN
= 0V CURRENT FLOWS INTO OUTPUT PIN V
OUT
= V
ADJ
(LT1962)
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