2020.01.01
There is a SOA (Safe Operating Area) for each product; if operation is within this area, it can be judged safe for use.
Example: When VDS = 20 V, Idpeak = 2 A, Pw = 100 μs → operation is in the Pw = 100 μs area, so use is possible.
A graph like that shown here appears on the web page of each Zener diode product. As an example, if the product being used is in the UDZS series, the allowable dissipation is 200 mW at an ambient temperature of 25℃, and is 100 mW at 87.5℃.
However, the allowable dissipation varies depending on the mounting board, and appropriate care should be taken.
During operation of the digital transistor, a base current is flowing in the forward direction between the emitter and base (E-B) of the internal transistor, and so a forward voltage (approx. 0.7 V at 25 ℃) appears across E-B. Because a resistor R2 is connected between E and B of the internal transistor in the digital transistor, the 0.7 V is also applied to R2. Hence we see that a current IR2 = 0.7 V/10 kΩ = 70 µA is flowing in R2.
When the input voltage Vin is 5 V, the potential at the IN pin is 5 V and the internal transistor E-B voltage difference is 0.7 V, so that a voltage of 5 V – 0.7 V = 4.3 V appears across both ends of the resistor R1. Hence we see that a current IR1 = 4.3 V/10 kΩ= 430 uA is flowing in R1.
Therefore we see that a current of 430 µA = 70 µA = 360 µA is flowing in the base of the internal transistor.
In this way we can calculate the base current flowing in the internal transistor. In order to turn on the digital transistor adequately (that is, lower the output voltage Vo(on)), the output current Io and input voltage Vin should be adjusted such that the output current Io is less than about 10 to 20 times the base current entering the internal transistor. If the input voltage Vin is inadequate and a sufficient output current cannot be passed, use a digital transistor with a smaller input resistance R1.
When the temperature is 25°C, the emitter-base forward voltage is about 0.7 V, but if there is a change in the temperature, the forward voltage drops by about 2.2 mV for every 1°C rise in temperature, so that when the temperature is for example 50°C, the voltage becomes about 0.7 V – (50°C-25°C)×2.2 mV = 0.645 V. Conversely, if the temperature drops to -40°C, the voltage is approximately 0.7 V + (25°C-(-40°C))×2.2 mV = 0.843 V.
In this way, the forward voltage VF changes with the temperature, and so appropriate care should be taken. Moreover, the forward voltage of 0.7 V at 25°C is merely a representative value. The voltage may vary within the range ±0.1 V, and so again, caution is required.
In the case of digital transistors, there is variation of approx. ±30% in the values of the internal resistances R1 and R2, and so the worst case should be considered when calculating resistance values.
Thus there is some variation in the forward voltage and in resistance values, and so the above calculation methods should be considered to be no more than guidelines.
Similarly to the above devices, voltage of up to about 5 V can be applied in the reverse direction across the collector and emitter (OUT-GND) of a digital transistor as well, but when a resistor is present between GND and IN, a current flows through this resistor.
Here transistor operation is compared for voltage input and for current input.
Voltage control Input: Emitter-base voltage VEB |
Current control Input: Base current IB |
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Measurement circuit diagram | ![]() |
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Theoretical equations | ![]() |
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Input-output characteristics | ![]() |
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On observing the input-output characteristic, whereas under current control, shown on the right side, the output changes linearly with the input, it is seen that under voltage control, shown on the left, the output changes exponentially with the input. In other words, when under voltage control, even a very small change in input causes a large change in the output current, so that operation becomes unstable.
For example, in the graph on the right side, when the input current is doubled from 40 µA to 80 µA, the output current doubles from 9 mA to 18 mA; but in the graph on the left side, a slight change of 14% in the input voltage, from 0.7 V to 0.8 V, causes the output current to increase seven-fold, from 10 mA to 70 mA.
Here, a slight amount of noise in the input voltage can cause a large change in the output current, making such a device unsuited to actual use.
Thus a bipolar transistor is more stable under current control, and so the input resistor R1 is necessary in order to convert the voltage output from the IC into a base current. A digital transistor incorporates this R1 internally, and so is effective for reducing the number of components and the amount of space required.
■About the resistor R2
・Role of resistor R2: To absorb leak currents and prevent malfunction
The resistor R2 prevents malfunctioning of the transistor by dropping to ground any leak currents, noise and the like that have entered from the input side.
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Leak currents enter transistor base as-is, transistor turns on. | All currents are dropped to GND, and no current flows to transistor base, so the transistor does not turn on. |
Any minute input currents are all dropped to ground, but if the input current becomes large, a part of the input current begins to enter the transistor base, and the transistor is turned on. | |
Input current is small When the input current is small, all of the input current is dropped to ground, and the transistor is not turned on. (There is no malfunctioning due to leak currents or the like) |
Input current becomes large When the input current becomes large, a part of the input current enters the base, and the transistor is turned on. (The transistor enters the normal on state.) |
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VR2=VBE<(forward-direction EB voltage ≒ 0.7 V) | VR2=VBE>(forward-direction EB voltage ≒ 0.7 V) |
The allowable losses (Pc) must be alleviated (derating) according to the ambient temperature (Ta). From the following graph, the power applied to the transistor should be reduced according to the ambient temperature.
Derating is also necessary in the SOA (Safe Operating Area); for details, please refer to “Before Using ROHM Transistor”. Moreover, electrical characteristics, such as the input voltage (VBE, VI(on), VI(off)), hFE, GI and so on for bipolar transistors and digital transistors, fluctuate with the temperature. Designs should employ electrical characteristic curve graphs to ensure that no problems arise in operation even when the temperature changes. The same precautions should be taken for MOSFETs as well.
This is the thermal resistance value until heat generated by a PN junction (or Schottky junction) of a silicon device is dissipated; Rth(j-a) represents the thermal resistance value from the junction to the periphery, Rth(j-c) is the value from the junction to the case, and Rth(j-l) is the value from the junction to the lead pins. A graph like the following appears on the web page of each product, and can be used to find the junction temperature during use Tj.
However, the thermal resistance value varies depending on the size and materials of the board, land patterns and the like, and appropriate care should be taken.
Downloadable materials, including lecture materials from ROHM-sponsored seminars and a selection guide for DC-DC converters, are now available.
Downloadable materials, including lecture materials from ROHM-sponsored seminars and a selection guide for DC-DC converters, are now available.