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OPA621 Datasheet(PDF) 14 Page - Texas Instruments |
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OPA621 Datasheet(HTML) 14 Page - Texas Instruments |
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14 / 17 page ![]() ® OPA621 14 defined as the change in degrees of the closed-loop phase over the same output voltage change. Both DG and DP are specified at the NTSC sub-carrier frequency of 3.58MHz. DG and DP increase with closed-loop gain and output voltage transition as shown in the Typical Performance Curves. All measurements were performed using a Tektronix model VM700 Video Measurement Set. DISTORTION The OPA621’s Harmonic Distortion characteristics into a 50 Ω load are shown vs frequency and power output in the Typical Performance Curves. Distortion can be further improved by increasing the load resistance as illustrated in Figure 8. Remember to include the contribution of the feedback resistance when calculating the effective load resistance seen by the amplifier. FIGURE 9. Two-Tone Third-Order Intermodulation Inter- cept vs Frequency. FIGURE 8. 10MHz Harmonic Distortion vs Load Resistance. Two-tone, third-order intermodulation distortion (IM) is an important parameter for many RF amplifier applications. Figure 9 shows the OPA621’s two-tone, third-order IM intercept vs frequency. For these measurements, tones were spaced 1MHz apart. This curve is particularly useful for determining the magnitude of the third-order IM products as a function of frequency, load resistance, and gain. For example, assume that the application requires the OPA621 to operate in a gain of +2V/V and drive 2Vp-p (4dBm for each tone) into 50 Ω at a frequency of 10MHz. Referring to Figure 9 we find that the intercept point is +47dBm. The magnitude of the third-order IM products can now be easily calculated from the expression: Third IMD = 2(OPI3P – PO) where OPI3P = third-order output intercept, dBm P O = output level/tone, dBm/tone Third IMD = third-order intermodulation ratio below each output tone, dB For this case OPI3P = 47dBm, P O = 4dBm, and the third- order IMD = 2(47 – 4) = 86dB below either 4dBm tone. The OPA621’s low IMD makes the device an excellent choice for a variety of RF signal processing applications. NOISE FIGURE The OPA621’s voltage and current noise spectral densities are specified in the Typical Performance Curves. For RF applications, however, Noise Figure (NF) is often the preferred noise specification since it allows system noise performance to be more easily calculated. The OPA621’s Noise Figure vs Source Resistance is shown in Figure 10. SPICE MODELS Computer simulation using SPICE is often useful when analyzing the performance of analog circuits and systems. This is particularly true for Video and RF amplifier circuits where parasitic capacitance and inductance can have a major effect on circuit performance. A SPICE model using MicroSim Corporation’s PSpice is available for the OPA621. This simulation model is available through the Burr-Brown web site at www.burr-brown.com or by calling the Burr- Brown Applications Department. NOISE FIGURE vs SOURCE RESISTANCE 25 20 15 10 5 0 10 100 1k 10k 100k Source Resistance ( ) Ω NFdB = 10log 1 + en2 + (inRS)2 4kTRS FIGURE 10. Noise Figure vs Source Resistance. V = 2Vp-p O 10MHz HARMONIC DISTORTION vs LOAD RESISTANCE –40 –50 –60 –70 –80 –90 0 100 200 300 400 500 Load Resistance ( ) Ω 3f 2f G = +2V/V G = +5V/V P OUT 250 Ω 250 Ω R L – + G = +2V/V 0 10203040 5060708090 100 10 15 20 25 30 35 40 45 50 55 60 Frequency (MHz) R = 50 L Ω R = 100 L Ω R = 400 L Ω |
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