TSH330 1.1 GHz Low-Noise Operational Amplifier ■ ■ ■ ■ ■ ■ ■ Bandwidth: 1.1GHz (Gain=+2) Quiescent current: 16.6 mA Slew rate: 1800V/µs Input noise: 1.3nV/√Hz Distortion: SFDR = -78dBc (10MHz, 2Vp-p) Output stage optimized for driving 100Ω loads Tested on 5V power supply Pin Connections (top view) D SO-8 (Plastic Micropackage) Description The TSH330 is a current feedback operational amplifier using a very high-speed complementary technology to provide a large bandwidth of 1.1GHz in gain of 2 while drawing only 16.6mA of quiescent current. In addition, the TSH330 offers 0.1dB gain flatness up to 160MHz with a gain of 2. With a slew rate of 1800V/µs and an output stage optimized for driving a standard 100Ω load, this device is highly suitable for applications where speed and low-distortion are the main requirements. 8 NC NC 1 -IN 2 _ 7 +VCC +IN 3 + 6 Output 5 NC -VCC 4 SO8 The TSH330 is a single operator available in the SO8 plastic package, saving board space as well as providing excellent thermal and dynamic performances. Applications ■ ■ ■ Communication & video test equipment Medical instrumentation ADC drivers Order Codes Part Number Temperature Range Package Conditioning Marking TSH330ID TSH330IDT -40°C to +85°C SO8 SO8 Tube Tape&Reel TSH330I TSH330I June 2005 Revision 3 1/19 TSH330 Absolute Maximum Ratings 1 Absolute Maximum Ratings Table 1. Key parameters and their absolute maximum ratings Symbol VCC Vid Vin Parameter Supply Voltage 1 Differential Input Voltage2 Range3 Value Unit 6 V +/-0.5 V +/-2.5 V Toper Input Voltage Operating Free Air Temperature Range -40 to + 85 °C Tstg Storage Temperature -65 to +150 °C Maximum Junction Temperature 150 °C Rthja SO8 Thermal Resistance Junction to Ambient 60 °C/W Rthjc SO8 Thermal Resistance Junction to Case 28 °C/W Tj Pmax 4 830 mW 5 2 kV 0.6 kV MM: Machine Model 6 (pins 1, 4, 5, 6, 7 and 8) MM: Machine Model (pins 2 and 3) CDM: Charged Device Model (pins 1, 4, 5, 6, 7 and 8) CDM: Charged Device Model (pins 2 and 3) Latch-up Immunity 200 V 80 1.5 1 200 V kV kV mA SO8 Maximum Power Dissipation (@Ta=25°C) for Tj=150°C HBM: Human Body Model (pins 1, 4, 5, 6, 7 and 8) HBM: Human Body Model (pins 2 and 3) ESD 1) All voltages values are measured with respect to the ground pin. 2) Differential voltage are non-inverting input terminal with respect to the inverting input terminal. 3) The magnitude of input and output voltage must never exceed VCC +0.3V. 4) Short-circuits can cause excessive heating. Destructive dissipation can result from short circuit on amplifiers. 5) Human body model, 100pF discharged through a 1.5kΩ resistor into pMin of device. 6) This is a minimum Value. Machine model ESD, a 200pF cap is charged to the specified voltage, then discharged directly into the IC with no external series resistor (internal resistor < 5Ω), into pin to pin of device. Table 2. Operating conditions Symbol VCC Vicm Parameter Supply Voltage 1 Common Mode Input Voltage 1) Tested in full production at 5V (±2.5V) supply voltage. 2/19 Value Unit 4.5 to 5.5 V -Vcc+1.5V, +Vcc-1.5V V Electrical Characteristics TSH330 2 Electrical Characteristics Table 3. Electrical characteristics for VCC= ±2.5Volts, Tamb=+25°C (unless otherwise specified) Symbol Parameter Test Condition Min. Typ. Max. -3.1 0.18 +3.1 Unit DC performance Vio Input Offset Voltage Offset Voltage between both inputs ∆Vio Vio drift vs. Temperature Tamb Tmin. < Tamb < Tmax. 0.8 Tmin. < Tamb < Tmax. 1.6 Iib+ Non Inverting Input Bias Current Tamb DC current necessary to bias the input + Tmin. < Tamb < Tmax. 26 Iib- Inverting Input Bias Current Tamb DC current necessary to bias the input Tmin. < Tamb < Tmax. 7 CMR SVR PSR ICC mV µV/°C 55 21 22 13 µA µA Common Mode Rejection Ratio ∆Vic = ±1V 20 log (∆Vic/∆Vio) Tmin. < Tamb < Tmax. Supply Voltage Rejection Ratio ∆Vcc= 3.5V to 5V 20 log (∆Vcc/∆Vout) Tmin. < Tamb < Tmax. Power Supply Rejection Ratio ∆Vcc=200mVp-p@1kHz 56 20 log (∆Vcc/∆Vout) Tmin. < Tamb < Tmax. 52 Supply Current DC consumption with no input signal No load 16.6 Tmin. < Tamb < Tmax. 16.6 mA 153 kΩ 152 kΩ 1500 1100 630 600 MHz 50 54 dB 54 63 74 dB 67 dB 20.2 mA Dynamic performance and output characteristics ROL Bw Transimpedance Output Voltage/Input Current Gain in open loop of a CFA. For a VFA, the analog of this feature is the Open Loop Gain (AVD) -3dB Bandwidth Frequency where the gain is 3dB below the DC gain AV Note: Gain Bandwidth Product criterion is not applicable for Current-FeedbackAmplifiers ∆Vout= ±1V, RL = 100Ω 104 Tmin. < Tamb < Tmax. Vout=20mVp-p, RL = 100Ω AV = +1 AV = +2 AV = -4 AV = -4, Tmin. < Tamb < Tmax. 550 Gain Flatness @ 0.1dB Small Signal Vout=20mVp-p Band of frequency where the gain varia- AV = +2, RL = 100Ω tion does not exceed 0.1dB SR VOH VOL Slew Rate Maximum output speed of sweep in large signal Vout = 2Vp-p, AV = +2, RL = 100Ω High Level Output Voltage RL = 100Ω Low Level Output Voltage 160 1.5 1800 V/µs 1.64 V Tmin. < Tamb < Tmax. 1.54 RL = 100Ω -1.55 Tmin. < Tamb < Tmax. -1.5 -1.5 V 3/19 TSH330 Electrical Characteristics Table 3. Electrical characteristics for VCC= ±2.5Volts, Tamb=+25°C (unless otherwise specified) Symbol Iout Parameter Isink Short-circuit Output current coming in the op-amp. See fig-17 for more details Isource Output current coming out from the opamp. See fig-18 for more details Test Condition Output to GND Min. Typ. 360 453 Tmin. < Tamb < Tmax. Max. Unit 427 Output to GND -340 Tmin. < Tamb < Tmax. mA -400 -350 Noise and distortion eN iN SFDR Equivalent Input Noise Voltage see application note on page 13 F = 100kHz Equivalent Input Noise Current (+) see application note on page 13 F = 100kHz Equivalent Input Noise Current (-) see application note on page 13 F = 100kHz Spurious Free Dynamic Range The highest harmonic of the output spectrum when injecting a filtered sine wave AV = +2, Vout = 2Vp-p, RL = 100Ω F = 10MHz F = 20MHz F = 100MHz F = 150MHz 1.3 nV/√Hz 22 pA/√Hz 16 pA/√Hz -78 -73 -48 -37 dBc Table 4. Closed-loop gain and feedback components VCC (V) Gain Rfb (Ω) -3dB Bw (MHz) 0.1dB Bw (MHz) +10 200 280 50 -10 200 270 45 +2 300 1000 160 -2 270 530 180 +1 300 1500 38 -1 260 600 280 ±2.5 4/19 Electrical Characteristics TSH330 24 22 20 18 16 14 12 10 8 6 4 2 0 -2 -4 Small Signal -6 Vcc=5V -8 Load=100 Ω -10 1M Figure 4. Frequency response, negative gain Gain=+10 Gain=+4 Gain (dB) Gain (dB) Figure 1. Frequency response, positive gain Gain=+2 Gain=+1 10M 100M 1G 24 22 20 18 16 14 12 10 8 6 4 2 0 -2 -4 Small Signal -6 Vcc=5V -8 Load=100Ω -10 1M Gain=-10 Gain=-4 Gain=-2 Gain=-1 10M Frequency (Hz) 100M 1G Frequency (Hz) Figure 2. Gain flatness, gain=+4 Figure 5. Gain flatness, gain=+2 12,2 6,2 Gain Flatness (dB) Gain Flatness (dB) 12,0 11,8 Vin Vout + - 11,6 8k2 22pF 300R 100R 6,0 Vin Vout + 5,8 - 8k2 1pF 300R 300R 5,6 11,4 Gain=+4, Vcc=5V, Small Signal 1M Gain=+2, Vcc=5V, Small Signal 10M 5,4 1M 100M 10M 10 16 8 14 6 12 4 10 2 8 0 6 -2 4 -4 Vin -8 - -10 -12 -14 Vout + 8k2 1pF -20 -22 1M 2 0 Vin Vout + -2 - -4 -6 300R 300R -8 8k2 22pF 300R 100R -10 -16 -18 1G Figure 6. Compensation, gain=+4 Gain (dB) Gain (dB) Figure 3. Compensation, gain=+2 -6 100M Frequency (Hz) Frequency (Hz) -12 Gain=+2, Vcc=5V, Small Signal 10M -14 100M Frequency (Hz) 1G -16 1M Gain=+4, Vcc=5V, Small Signal 10M 100M 1G Frequency (Hz) 5/19 TSH330 Electrical Characteristics Figure 7. Compensation, gain=+10 Figure 10. Quiescent current vs. Vcc 24 20 22 15 20 18 Icc(+) 10 16 5 12 10 Vin 8 + 6 - 4 15pF 2 Icc (mA) Gain (dB) 14 Vout 200R 22R 0 -5 -10 -15 0 -20 -2 Gain=+10, Vcc=5V, Small Signal -4 -6 -8 1M -25 10M 100M -30 1,25 1G Icc(-) Gain=+2 Vcc=5V Input to ground, no load 1,50 1,75 Frequency (Hz) 2,00 2,25 2,50 +/-Vcc (V) Figure 8. Input current noise vs. frequency Figure 11. Input voltage noise vs. frequency 150 4.0 140 130 120 110 3.5 Neg. Current Noise 90 80 3.0 en (nV/VHz) in (pA/VHz) 100 Pos. Current Noise 70 60 50 2.5 2.0 40 30 1.5 20 10 1k 10k 100k 1M 1.0 1k 10M 10k Frequency (Hz) 100k 1M 10M Frequency (Hz) Figure 9. Output amplitude vs. load Figure 12. Noise figure 40 4,0 35 30 25 NF (dB) Vout max. (Vp-p) 3,5 3,0 20 15 10 2,5 Freq=? Gain=+2 Vcc=5V 2,0 10 100 1k Load (ohms) 6/19 10k 100k 5 Vcc=5V 0 1 10 100 1k Rsource (ohms) 10k 100k Electrical Characteristics TSH330 Figure 13. Output amplitude vs. frequency Figure 16. Distortion vs. amplitude 5 -20 -25 -30 -35 4 HD2 & HD3 (dBc) Vout max. (Vp-p) -40 3 2 1 -45 HD2 -50 -55 -60 -65 -70 -75 -80 Gain=+2 Vcc=5V F=30MHz Load=100 Ω -85 Gain=+2 Vcc=5V Load=100Ω -90 HD3 -95 -100 0 1M 10M 100M 0 1G 1 Figure 14. Distortion vs. amplitude 600 -25 550 -30 500 -35 4 -0,5 0,0 +2.5V VOL -45 400 Isink (mA) -50 -55 -60 HD2 -70 350 withou t load + -1V Isink _ 450 -40 HD2 & HD3 (dBc) 3 Figure 17. Isink -20 -65 2 Output Amplitude (Vp-p) Frequency (Hz) V - 2.5V RG Amplifier in open loop without load 300 250 200 -75 -80 HD3 -90 150 Gain=+2 Vcc=5V F=10MHz Load=100Ω -85 -95 100 50 0 -2,0 -100 0 1 2 3 4 -1,5 -1,0 V (V) Output Amplitude (Vp-p) Figure 15. Distortion vs. amplitude Figure 18. Isource -20 0 -25 -50 -30 -100 -35 -150 -45 Isource (mA) HD2 & HD3 (dBc) -40 -50 HD2 -55 -60 -65 -70 -75 -80 HD3 -90 -95 1 2 Output Amplitude (Vp-p) 3 -300 +2.5V VOH -350 without load + +1V -400 Isource _ V - 2.5V RG -500 Amplifier in open loop without load -550 -100 0 -250 -450 Gain=+2 Vcc=5V F=20MHz Load=100Ω -85 -200 4 -600 0,0 0,5 1,0 1,5 2,0 V (V) 7/19 TSH330 Electrical Characteristics Figure 19. Slew rate Figure 22. CMR vs. temperature 64 2,0 Output Response (V) 62 60 1,5 CMR (dB) 58 1,0 0,5 56 54 52 50 Gain=+2 Vcc=5V Load=100Ω 0,0 -2ns -1ns 0s 1ns 2ns 48 46 Gain=+1 Vcc=5V Load=100Ω 3ns -40 Time (ns) -20 0 20 40 60 80 100 120 80 100 120 80 100 120 Temperature (°C) Figure 20. Reverse isolation vs. frequency Figure 23. SVR vs. temperature 85 0 80 -20 SVR (dB) 75 Gain (dB) -40 -60 70 65 60 -80 Small Signal Vcc=5V Load=100Ω -100 1M 55 Gain=+1 Vcc=5V Load=100Ω 50 10M 100M 1G -40 -20 0 Frequency (Hz) 20 40 60 Temperature (°C) Figure 21. Bandwidth vs. temperature Figure 24. ROL vs. temperature 1,3 200 1,2 180 1,0 ROL (MΩ ) Bw (GHz) 1,1 0,9 0,8 160 140 0,7 0,6 120 Gain=+2 Vcc=5V Load=100Ω Open Loop Vcc=5V 0,5 100 -40 -20 0 20 40 60 Temperature (°C) 8/19 80 100 120 -40 -20 0 20 40 60 Temperature (°C) Electrical Characteristics TSH330 Figure 25. I-bias vs. temperature Figure 28. Icc vs. temperature 20 24 15 Ib(+) 22 Icc(+) 10 20 5 0 ICC (mA) IBIAS (µA) 18 16 14 Ib(-) Icc(-) -20 10 6 -10 -15 12 8 -5 Gain=+1 Vcc=5V no Load -30 In+/In- to GND -25 Gain=+1 Vcc=5V Load=100 Ω -35 -40 -20 0 20 40 60 80 100 120 -40 -20 0 Temperature (°C) 20 40 60 80 100 120 80 100 120 Temperature (°C) Figure 26. Vio vs. temperature Figure 29. Iout vs. temperature 1000 600 400 Isource 800 Iout (mA) VIO (micro V) 200 600 400 0 -200 Isink -400 200 Open Loop Vcc=5V Load=100Ω -600 0 -40 -20 0 20 40 60 80 100 120 Temperature (°C) Output: short-circuit Gain=+1 Vcc=5V -800 -40 -20 0 20 40 60 Temperature (°C) Figure 27. VOH & VOL vs. temperature 2 V OH VOH & OL (V) 1 0 -1 VOL -2 -3 Gain=+1 Vcc=5V Load=100Ω -4 -40 -20 0 20 40 60 80 Temperature (°C) 9/19 TSH330 Evaluation Boards 3 Evaluation Boards An evaluation board kit optimized for high-speed operational amplifiers is available (order code: KITHSEVAL/STDL). The kit includes the following evaluation boards, as well as a CD-ROM containing datasheets, articles, application notes and a user manual: z SOT23_SINGLE_HF BOARD: Board for the evaluation of a single high-speed op-amp in SOT23-5 package. z SO8_SINGLE_HF: Board for the evaluation of a single high-speed op-amp in SO8 package. z SO8_DUAL_HF: Board for the evaluation of a dual high-speed op-amp in SO8 package. z SO8_S_MULTI: Board for the evaluation of a single high-speed op-amp in SO8 package in inverting and non-inverting configuration, dual and single supply. z SO14_TRIPLE: Board for the evaluation of a triple high-speed op-amp in SO14 package with video application considerations. Board material: z 2 layers z FR4 (εr=4.6) z epoxy 1.6mm z copper thickness: 35µm Figure 30. Evaluation kit for high-speed op-amps 10/19 Power Supply Considerations TSH330 4 Power Supply Considerations Correct power supply bypassing is very important for optimizing performance in high-frequency ranges. Bypass capacitors should be placed as close as possible to the IC pins to improve high-frequency bypassing. A capacitor greater than 1µF is necessary to minimize the distortion. For better quality bypassing, a capacitor of 10nF can be added using the same implementation conditions. Bypass capacitors must be incorporated for both the negative and the positive supply. For example, on the SO8_SINGLE_HF board, these capacitors are C6, C7, C8, C9. Figure 31. Circuit for power supply bypassing +VCC 10microF + 10nF + - 10nF 10microF + -VCC Single power supply In the event that a single supply system is used, new biasing is necessary to assume a positive output dynamic range between 0V and +VCC supply rails. Considering the values of VOH and VOL, the amplifier will provide an output dynamic from +0.9V to +4.1V on 100Ω load. The amplifier must be biased with a mid-supply (nominally +VCC/2), in order to maintain the DC component of the signal at this value. Several options are possible to provide this bias supply, such as a virtual ground using an operational amplifier or a two-resistance divider (which is the cheapest solution). A high resistance value is required to limit the current consumption. On the other hand, the current must be high enough to bias the non-inverting input of the amplifier. If we consider this bias current (55µA max.) as the 1% of the current through the resistance divider to keep a stable mid-supply, two resistances of 470Ω can be used. The input provides a high pass filter with a break frequency below 10Hz which is necessary to remove the original 0 volt DC component of the input signal, and to fix it at +VCC/2. Figure 32 illustrates a 5V single power supply configuration for the SO8_SINGLE evaluation board (see Evaluation Boards on page 10). 11/19 TSH330 Power Supply Considerations A capacitor CG is added in the gain network to ensure a unity gain in low-frequency to keep the right DC component at the output. CG contributes to a high-pass filter with Rfb//RG and its value is calculated with a consideration of the cut off frequency of this low-pass filter. Figure 32. Circuit for +5V single supply +5V 10µF + IN +5V Rin 1kΩ 100µF _ 100Ω R1 470Ω Rfb R2 470Ω 12/19 + 1µF RG 10nF + CG OUT Noise Measurements TSH330 5 Noise Measurements The noise model is shown in Figure 33, where: z eN: input voltage noise of the amplifier z iNn: negative input current noise of the amplifier z iNp: positive input current noise of the amplifier Figure 33. Noise model + iN+ R3 output HP3577 Input noise: 8nV/√Hz _ N3 iN- eN R2 N2 R1 N1 The thermal noise of a resistance R is: 4kTR ∆ F where ∆F is the specified bandwidth. On a 1Hz bandwidth the thermal noise is reduced to 4kTR where k is the Boltzmann's constant, equal to 1,374.10-23J/°K. T is the temperature (°K). The output noise eNo is calculated using the Superposition Theorem. However eNo is not the simple sum of all noise sources, but rather the square root of the sum of the square of each noise source, as shown in Equation 1: eNo = eN o 2 2 2 2 2 2 2 V1 + V2 + V3 + V 4 + V5 + V6 2 2 2 2 2 2 2 R2 2 R2- 2 × 4kTR3 = e N × g + iNn × R 2 + iNp × R3 × g + -------- × 4kTR1 + 4kTR2 + 1 + ------R1 R1 Equation 1 Equation 2 13/19 TSH330 Noise Measurements The input noise of the instrumentation must be extracted from the measured noise value. The real output noise value of the driver is: eNo = 2 2 ( Measured ) – ( instrumentation ) Equation 3 The input noise is called the Equivalent Input Noise as it is not directly measured but is evaluated from the measurement of the output divided by the closed loop gain (eNo/g). After simplification of the fourth and the fifth term of Equation 2 we obtain: eNo 2 2 2 2 2 2 2 2 R2 2 = eN × g + iNn × R2 + iNp × R3 × g + g × 4kTR2 + 1 + -------- × 4kTR3 R1 Equation 4 Measurement of the Input Voltage Noise eN If we assume a short-circuit on the non-inverting input (R3=0), from Equation 4 we can derive: eNo = 2 2 2 2 eN × g + iNn × R2 + g × 4kTR2 Equation 5 In order to easily extract the value of eN, the resistance R2 will be chosen to be as low as possible. In the other hand, the gain must be large enough: R3=0, gain: g=100 Measurement of the Negative Input Current Noise iNn To measure the negative input current noise iNn, we set R3=0 and use Equation 5. This time the gain must be lower in order to decrease the thermal noise contribution: R3=0, gain: g=10 Measurement of the Positive Input Current Noise iNp To extract iNp from Equation 3, a resistance R3 is connected to the non-inverting input. The value of R3 must be chosen in order to keep its thermal noise contribution as low as possible against the iNp contribution: R3=100W, gain: g=10 14/19 Intermodulation Distortion Product TSH330 6 Intermodulation Distortion Product The non-ideal output of the amplifier can be described by the following series: 2 n Vout = C 0 + C 1 Vin + C 2 V in + … Cn V in due to non-linearity in the input-output amplitude transfer, where the input is Vin=Asinωt, C0 is the DC component, C1(Vin) is the fundamental and Cn is the amplitude of the harmonics of the output signal Vout. A one-frequency (one-tone) input signal contributes to harmonic distortion. A two-tone input signal contributes to harmonic distortion and to the intermodulation product. The study of the intermodulation and distortion for a two-tone input signal is the first step in characterizing the driving capability of multi-tone input signals. In this case: Vin = A sin ω 1 t + A sin ω 2 t then: 2 n V out = C 0 + C1 ( A sin ω 1 t + A sin ω 2 t ) + C 2 ( A sin ω 1 t + A sin ω 2 t ) … + C n ( A sin ω 1 t + A sin ω 2 t ) From this expression, we can extract the distortion terms, and the intermodulation terms form a single sine wave: second-order intermodulation terms IM2 by the frequencies (ω1-ω2) and (ω1+ω2) with an amplitude of C2A2 and third-order intermodulation terms IM3 by the frequencies (2ω1-ω2), (2ω1+ω2), (− ω1+2ω2) and (ω1+2ω2) with an amplitude of (3/4)C3A3. The measurement of the intermodulation product of the driver is achieved by using the driver as a mixer by a summing amplifier configuration (see Figure 34). In this way, the non-linearity problem of an external mixing device is avoided. Figure 34. Inverting summing amplifier (using evaluation board SO8_S_MULTI) Vin1 R1 Vin2 R2 R fb _ Vout + 100Ω R 15/19 TSH330 The Bias of an Inverting Amplifier 7 The Bias of an Inverting Amplifier A resistance is necessary to achieve a good input biasing, such as resistance R shown in Figure 35. The magnitude of this resistance is calculated by assuming the negative and positive input bias current. The aim is to compensate for the offset bias current, which could affect the input offset voltage and the output DC component. Assuming Ib-, Ib+, Rin, Rfb and a zero volt output, the resistance R will be: R in × R fb R = ---------------------R in + R fb Figure 35. Compensation of the input bias current Rfb Ib- Rin _ Vcc+ Output + Vcc- Ib+ R 16/19 Load Active Filtering TSH330 8 Active Filtering Figure 36. Low-pass active filtering, Sallen-Key C1 R1 R2 + IN OUT C2 _ 100Ω Rfb RG From the resistors Rfb and RG we can directly calculate the gain of the filter in a classical non-inverting amplification configuration: R fb A V = g = 1 + ---------Rg We assume the following expression as the response of the system: Voutj ω g T j ω = ------------------- = --------------------------------------------Vin j ω 2 jω ( jω) 1 + 2 ζ ------- + -------------ω c ω 2 c The cut-off frequency is not gain-dependent and so becomes: ω 1 c = ------------------------------------R1R2C 1C2 The damping factor is calculated by the following expression: 1 ζ = --- ω c ( C 1 R1 + C 1 R2 + C 2 R 1 – C 1 R 1 g ) 2 The higher the gain, the more sensitive the damping factor is. When the gain is higher than 1, it is preferable to use some very stable resistor and capacitor values. In the case of R1=R2=R: R fb 2 C 2 – C1 ---------Rg ζ = -----------------------------------2 C1 C2 Due to a limited selection of values of capacitors in comparison with resistors, we can fix C1=C2=C, so that: R fb 2 R 2 – R1 ---------Rg ζ = -----------------------------------2 R1 R2 17/19 TSH330 Package Mechanical Data 9 Package Mechanical Data SO-8 MECHANICAL DATA DIM. mm. MIN. TYP inch MAX. MIN. TYP. MAX. A 1.35 1.75 0.053 0.069 A1 0.10 0.25 0.04 0.010 A2 1.10 1.65 0.043 0.065 B 0.33 0.51 0.013 0.020 C 0.19 0.25 0.007 0.010 D 4.80 5.00 0.189 0.197 E 3.80 4.00 0.150 0.157 e 1.27 0.050 H 5.80 6.20 0.228 0.244 h 0.25 0.50 0.010 0.020 L 0.40 1.27 0.016 0.050 k ddd 8˚ (max.) 0.1 0.04 0016023/C 18/19 Revision History TSH330 10 Revision History Date Revision Description of Changes Oct. 2004 1 First release corresponding to Preliminary Data version of datasheet. Dec. 2004 2 Release of mature product datasheet. June 2005 3 Table 1 on page 2 - Rthjc: Thermal Resistance Junction to Ambient replaced by Thermal Resistance Junction to Case Information furnished is believed to be accurate and reliable. However, STMicroelectronics assumes no responsibility for the consequences of use of such information nor for any infringement of patents or other rights of third parties which may result from its use. No license is granted by implication or otherwise under any patent or patent rights of STMicroelectronics. Specifications mentioned in this publication are subject to change without notice. This publication supersedes and replaces all information previously supplied. STMicroelectronics products are not authorized for use as critical components in life support devices or systems without express written approval of STMicroelectronics. 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