| Datenblatt-Suchmaschine für elektronische Bauteile |
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KH231AI Datenblatt(PDF) 5 Page - Cadeka Microcircuits LLC. |
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KH231AI Datenblatt(HTML) 5 Page - Cadeka Microcircuits LLC. |
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5 / 6 page ![]() KH231 DATA SHEET REV. 1A January 2004 5 θ ca = 65°C/W for the KH231 without heat sink in still air. 30°C/W for the KH231 with a Wakefield 215 heat sink in still air. 10°C/W for the KH231 with a Wakefield 215 heat sink at 300 ft/min air. 30°C/W for the KH231 with a Thermalloy 2240A heat sink in still air. 5°C/W for the KH231 with a Thermalloy 2240A heat sink at 500 ft/min air. For example, with the KH231 operating at ±15V while driving a 100 Ω load at 15V pp output (50% duty cycle pulse waveform, DC = 0), P(npn) = P(pnp) = 190mW (Rcol = 33) and P(cir) = 0.48W. Then with the Wakefield 215 heat sink and air flow of 300 ft/min the output transistors’ Tj is 28°C above ambient and worst case Tj in the rest of the circuit is 32°C above ambient. In still air, however, the rise in Tj is 45°C and 49°C, respectively. With no heat sink, the rise in Tj is 75°C and 79°C, respectively! Under most conditions, HEAT SINKING IS REQUIRED. Other methods of heat sinking may be used, but for best results, make contact with the base of the KH231 package, use a large thermal capacity heat sink and use forced air convection. Low VCC Operation: Supply Current Adjustment The KH231 is designed to operate on supplies as low as ±5V. In order to improve full bandwidth at reduced sup- ply voltages, the supply current (ICC) must be increased. The plot of Bandwidth vs. VCC, shows the effect of short- ing pins 1 and 2 and pins 8 and 9; this will increase both bandwidth and supply current. Care should be taken to not exceed the maximum junction temperatures; for this reason this technique should not be used with supplies exceeding ±10V. For intermediate values of VCC, external resistors between pins 1 and 2 and pins 8 and 9 can be used. Offset Voltage Adjustment If trimming of the input offset voltage (Vos = Vni -Vin) is desired, a resistor value of 10k Ω to 1MΩ placed between pins 8 and 9 will cause Vos to become more negative by 8mV to 0.2mV respectively. Similarly, a resistor placed between pins 1 and 2 will cause Vos, to become more positive. Thermal Considerations At high ambient temperatures or large internal power dissipations, heat sinking is required to maintain acceptable junction temperatures. Use the thermal model on the previous page to determine junction temperatures. Many styles of heat sinks are available for TO-8 packages; the Thermalloy 2240 and 2268 are good examples. Some heat sinks are the radial fin type which cover the pc board and may interfere with external components. An excellent solution to this problem is to use surface mounted resistors and capacitors. They have a very low profile and actually improve high frequency performance. For use of these heat sinks with conventional components, a 0.1” high spacer can be inserted under the TO-8 package to allow sufficient clearance. P(circuit) = (ICC)((+VCC) – (VCC)) where ICC = 16mA at ±15V P(xxx) = [(±VCC) – Vout – (Icol) (Rcol + 4)] (Icol) (%Duty) For positive Vo and VCC, this is the power in the npn device. For negative Vo and VCC, this is the power in the pnp device. Icol = Vo/RL or 4mA, whichever is greater. (Include feed- back R in RL.) Rcol is a resistor (33Ω recommended) between the xxx collector and ±VCC. The limiting factor for output current and voltage is junction temperature. Of secondary importance is I(out), which should not exceed 150mA. Tj(pnp) = P(pnp) (100 + θca) + (P(cir) + P(npn))(θca) + Ta, similar for Tj(npn). Tj(cir) = P(cir)(48 + θca) + (P(pnp) + P(npn))(θca) + Ta. + - Tambient θca Tcase 17.5 °C/W Tj(circuit) Pcircuit 100 °C/W Tj(npn) Pnpn 100 °C/W Ppnp Tj(pnp) |
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