LT6600CS8-2.5 [Linear]

Very Low Noise, Differential Amplifier and 2.5MHz Lowpass Filter; 非常低噪声,差分放大器和2.5MHz的低通滤波器
LT6600CS8-2.5
型号: LT6600CS8-2.5
厂家: Linear    Linear
描述:

Very Low Noise, Differential Amplifier and 2.5MHz Lowpass Filter
非常低噪声,差分放大器和2.5MHz的低通滤波器

运算放大器 放大器电路
文件: 总12页 (文件大小:169K)
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Final Electrical Specifications  
LT6600-2.5  
Very Low Noise, Differential  
Amplifier and 2.5MHz Lowpass Filter  
June 2003  
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FEATURES  
DESCRIPTIO  
Programmable Differential Gain via Two External  
The LT®6600-2.5 combines a fully differential amplifier  
with a 4th order 2.5MHz lowpass filter approximating a  
Chebyshev frequency response. Most differential amplifi-  
ers require many precision external components to tailor  
gain and bandwidth. In contrast, with the LT6600-2.5, two  
externalresistorsprogramdifferentialgain, andthefilter’s  
2.5MHz cutoff frequency and passband ripple are inter-  
nallyset.TheLT6600-2.5alsoprovidesthenecessarylevel  
shifting to set its output common mode voltage to accom-  
modate the reference voltage requirements of A/Ds.  
Resistors  
Adjustable Output Common Mode Voltage  
Operates and Specified with 3V, 5V, ±5V Supplies  
0.5dB Ripple 4th Order Lowpass Filter with 2.5MHz  
Cutoff  
86dB S/N with 3V Supply and 1VRMS Output  
Low Distortion, 1VRMS, 800Load  
1MHz: 95dBc 2nd, 88dBc 3rd  
Fully Differential Inputs and Outputs  
Compatible with Popular Differential Amplifier  
Using a proprietary internal architecture, the LT6600-2.5  
integrates an antialiasing filter and a differential amplifier/  
driver without compromising distortion or low noise  
performance. At unity gain the measured in band  
signal-to-noise ratio is an impressive 86dB. At higher  
gains the input referred noise decreases so the part can  
Pinouts  
SO-8 Package  
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APPLICATIO S  
High Speed ADC Antialiasing and DAC Smoothing in  
Networking or Cellular Base Station Applications  
High Speed Test and Measurement Equipment  
Medical Imaging  
Drop-in Replacement for Differential Amplifiers  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
process smaller input differential signals without signifi-  
cantly degrading the output signal-to-noise ratio.  
The LT6600-2.5 also features low voltage operation. The  
differential design provides outstanding performance for  
a4VP-P signallevelwhilethepartoperateswithasingle3V  
supply. The LT6600-2.5 is available in an SO-8 package.  
For similar devices with higher cutoff frequency, refer to  
the LT6600-10 and LT6600-20 data sheets.  
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TYPICAL APPLICATIO  
Amplitude Response  
12  
V
= ±2.5V  
S
0
–12  
–24  
–36  
–48  
–60  
–72  
–84  
–96  
5V  
0.1µF  
1580Ω  
3
1
7
2
8
+
V
V
IN  
IN  
4
+
V
OUT  
LT6600-2.5  
0.01µF  
1580Ω  
V
OUT  
5
+
6
660025 TA01a  
100k  
1M  
10M  
50M  
FREQUENCY (Hz)  
660025 TA01b  
660025i  
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 represen-  
tationthattheinterconnectionofitscircuitsasdescribedhereinwillnotinfringeonexistingpatentrights.  
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LT6600-2.5  
W W U W  
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ABSOLUTE AXI U RATI GS  
(Note 1)  
PACKAGE/ORDER I FOR ATIO  
Total Supply Voltage................................................ 11V  
Operating Temperature Range (Note 6) ...–40°C to 85°C  
Specified Temperature Range (Note 7)....–40°C to 85°C  
Junction Temperature........................................... 150°C  
Storage Temperature Range ................. 65°C to 150°C  
Lead Temperature (Soldering, 10 sec).................. 300°C  
ORDER PART  
TOP VIEW  
NUMBER  
+
IN  
1
2
3
4
8
7
6
5
IN  
V
V
LT6600CS8-2.5  
LT6600IS8-2.5  
OCM  
MID  
+
V
V
+
OUT  
OUT  
S8 PART MARKING  
S8 PACKAGE  
8-LEAD PLASTIC SO  
660025  
600I25  
TJMAX = 150°C, θJA = 100°C/W  
Consult LTC Marketing for parts specified with wider operating temperature ranges.  
ELECTRICAL CHARACTERISTICS  
The denotes specifications that apply over the full operating temperature  
range, otherwise specifications are at TA = 25°C. Unless otherwise specified VS = 5V (V+ = 5V, V= 0V), RIN = 1580, and RLOAD = 1k.  
PARAMETER  
Filter Gain, V = 3V  
CONDITIONS  
MIN  
– 0.5  
– 0.15  
– 0.2  
– 0.6  
2.1  
TYP  
0.1  
MAX  
0.4  
0.1  
0.6  
0.5  
0
UNITS  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
= 2V , f = DC to 260kHz  
P-P IN  
S
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
R
= 1580Ω  
= 2V , f = 700kHz (Gain Relative to 260kHz)  
0
IN  
P-P IN  
= 2V , f = 1.9MHz (Gain Relative to 260kHz)  
0.2  
P-P IN  
= 2V , f = 2.2MHz (Gain Relative to 260kHz)  
0.1  
P-P IN  
= 2V , f = 2.5MHz (Gain Relative to 260kHz)  
0.9  
P-P IN  
= 2V , f = 7.5MHz (Gain Relative to 260kHz)  
– 34  
– 51  
–0.1  
0
– 31  
P-P IN  
= 2V , f = 12.5MHz (Gain Relative to 260kHz)  
P-P IN  
Filter Gain, V = 5V  
= 2V , f = DC to 260kHz  
0.5  
– 0.15  
– 0.2  
– 0.6  
– 2.1  
0.4  
0.1  
0.6  
0.5  
0
S
P-P IN  
R
= 1580Ω  
= 2V , f = 700kHz (Gain Relative to 260kHz)  
IN  
P-P IN  
= 2V , f = 1.9MHz (Gain Relative to 260kHz)  
0.2  
P-P IN  
= 2V , f = 2.2MHz (Gain Relative to 260kHz)  
0.1  
P-P IN  
= 2V , f = 2.5MHz (Gain Relative to 260kHz)  
–0.9  
34  
51  
0.1  
P-P IN  
= 2V , f = 7.5MHz (Gain Relative to 260kHz)  
–31  
P-P IN  
= 2V , f = 12.5MHz (Gain Relative to 260kHz)  
P-P IN  
Filter Gain, V = ±5V  
= 2V , f = DC to 260kHz  
0.6  
0.4  
S
P-P IN  
Filter Gain, R = 402Ω  
V
V
V
= 2V , f = DC to 260kHz, V = 3V  
11.3  
11.3  
11.2  
11.8  
11.8  
11.7  
12.3  
12.3  
12.2  
dB  
dB  
dB  
IN  
IN  
IN  
IN  
P-P IN  
S
= 2V , f = DC to 260kHz, V = 5V  
P-P IN  
S
= 2V , f = DC to 260kHz, V = ±5V  
P-P IN  
S
Filter Gain Temperature Coefficient (Note 2)  
f
= 260kHz, V = 2V  
P-P  
780  
51  
ppm/C  
IN  
IN  
Noise  
Noise BW = 10kHz to 2.5MHz  
1MHz, 1V , R = 800Ω  
µV  
RMS  
Distortion (Note 4)  
2nd Harmonic  
3rd Harmonic  
95  
88  
dBc  
dBc  
RMS  
L
Differential Output Swing  
Input Bias Current  
Measured Between Pins 4 and 5  
Average of Pin 1 and Pin 8  
V = 5V  
S
8.8  
5.1  
9.3  
5.5  
V
V
S
P-P DIFF  
P-P DIFF  
V = 3V  
– 35  
15  
µA  
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LT6600-2.5  
ELECTRICAL CHARACTERISTICS  
The denotes specifications that apply over the full operating temperature  
range, otherwise specifications are at TA = 25°C. Unless otherwise specified VS = 5V (V+ = 5V, V= 0V), RIN = 1580, and RLOAD = 1k.  
PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
Input Referred Differential Offset  
R
IN  
= 1580Ω  
V = 3V  
5
5
5
25  
30  
35  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
R
IN  
= 402Ω  
V = 3V  
3
3
3
13  
16  
20  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
Differential Offset Drift  
10  
µV/°C  
Input Common Mode Voltage (Note 3)  
Differential Input = 500mV  
IN  
,
V = 3V  
0.0  
0.0  
–2.5  
1.5  
3.0  
1.0  
V
V
V
P-P  
S
R
= 402Ω  
V = 5V  
S
V = ±5V  
S
Output Common Mode Voltage (Note 5)  
Differential Input = 2V  
Pin 7 at Mid-Supply  
,
V = 3V  
1.0  
1.5  
–1.0  
1.5  
3.0  
2.0  
V
V
V
P-P  
S
V = 5V  
S
V = ±5V  
S
Output Common Mode Offset  
(with Respect to Pin 2)  
V = 3V  
–25  
–30  
–55  
10  
5
–10  
45  
45  
35  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
Common Mode Rejection Ratio  
63  
dB  
Voltage at V  
(Pin 7)  
V = 5V  
S
2.46  
4.3  
2.51  
1.5  
2.55  
7.7  
V
V
MID  
S
V = 3V  
V
V
Input Resistance  
Bias Current  
5.7  
kΩ  
MID  
V
= V = V /2  
V = 5V  
–15  
–10  
–3  
–3  
µA  
µA  
OCM  
OCM  
MID  
S
S
V = 3V  
S
Power Supply Current  
V = 3V, V = 5V  
26  
30  
33  
36  
mA  
mA  
mA  
S
S
V = 3V, V = 5V  
S
S
V = ±5V  
28  
S
Note 1: Absolute Maximum Ratings are those values beyond which the life  
of a device may be impaired.  
Note 2: This is the temperature coefficient of the internal feedback  
Note 5: Output common mode voltage is the average of the voltages at  
Pins 4 and 5. The output common mode voltage is equal to the voltage  
applied to Pin 2.  
resistors assuming a temperature independent external resistor (R ).  
Note 3: The input common mode voltage is the average of the voltages  
Note 6: Both the LT6600CS8-2.5 and LT6600IS8-2.5 are guaranteed  
functional over the operating temperature range of –40°C to 85°C.  
IN  
applied to the external resistors (R ). Specification guaranteed for  
Note 7: The LT6600CS8-2.5 is guaranteed to meet specified performance  
from 0°C to 70°C and is designed, characterized and expected to meet  
specified performance from –40°C and 85°C, but is not tested or QA  
sampled at these temperatures. The LT6600IS8-2.5 is guaranteed to meet  
specified performance from –40°C to 85°C.  
IN  
R
IN  
402.  
Note 4: Distortion is measured differentially using a single-ended  
stimulus. The input common mode voltage, the voltage at Pin 2, and the  
voltage at Pin 7 are equal to one half of the total power supply voltage.  
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LT6600-2.5  
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PI FU CTIO S  
INand IN+ (Pins 1, 8): Input Pins. Signals can be applied  
to either or both input pins through identical external  
resistors, RIN. The DC gain from differential inputs to the  
differential outputs is 1580/RIN.  
supply applications, bypass Pin 3 to ground and Pin 6 to  
ground with a quality 0.1µF ceramic capacitor.  
OUT+ and OUT(Pins 4, 5): Output Pins. Pins 4 and 5 are  
the filter differential outputs. Each pin can drive a 100Ω  
and/or 50pF load to AC ground.  
V
OCM (Pin 2): Is the DC Common Mode Reference Voltage  
for the 2nd Filter Stage. Its value programs the common  
mode voltage of the differential output of the filter. Pin 2 is  
a high impedance input, which can be driven from an  
external voltage reference, or Pin 2 can be tied to Pin 7 on  
the PC board. Pin 2 should be bypassed with a 0.01µF  
ceramiccapacitorunlessitisconnectedtoagroundplane.  
V+ and V(Pins 3, 6): Power Supply Pins. For a single  
3.3V or 5V supply (Pin 6 grounded) a quality 0.1µF  
ceramic bypass capacitor is required from the positive  
supply pin (Pin 3) to the negative supply pin (Pin 6). The  
bypass should be as close as possible to the IC. For dual  
V
MID (Pin 7): The VMID pin is internally biased at mid-  
supply, see block diagram. For single supply operation,  
the VMID pin should be bypassed with a quality 0.01µF  
ceramic capacitor to Pin 6. For dual supply operation, Pin  
7 can be bypassed or connected to a high quality DC  
ground. A ground plane should be used. A poor ground  
will increase noise and distortion. Pin 7 sets the output  
common mode voltage of the 1st stage of the filter. It has  
a 5.5kimpedance, and it can be overridden with an  
external low impedance voltage source.  
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LT6600-2.5  
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BLOCK DIAGRA  
R
IN  
+
+
V
IN  
IN  
V
OUT  
5
V
MID  
8
7
6
+
V
11k  
11k  
PROPRIETARY  
LOWPASS  
FILTER STAGE  
1580  
800Ω  
V
OP AMP  
800Ω  
800Ω  
+
+
OCM  
V
V
OCM  
+
+
800Ω  
1580Ω  
1
2
3
4
660025 BD  
+
+
V
V
IN  
IN  
OCM  
V
OUT  
R
IN  
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LT6600-2.5  
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APPLICATIO S I FOR ATIO  
Interfacing to the LT6600-2.5  
output voltage is 1.65V, and the differential output voltage  
is 2VP-P for frequencies below 2.5MHz. The common  
mode output voltage is determined by the voltage at pin 2.  
Since pin 2 is shorted to pin 7, the output common mode  
is the mid-supply voltage. In addition, the common mode  
input voltage can be equal to the mid-supply voltage of  
Pin 7.  
TheLT6600-2.5requirestwoequalexternalresistors,RIN,  
to set the differential gain to 1580/RIN. The inputs to the  
+
filter are the voltages VIN and VINpresented to these  
external components, Figure 1. The difference between  
VIN+ and VINis the differential input voltage. The average  
+
of VIN and VIN is the common mode input voltage.  
Similarly, the voltages VOUT+ and VOUTappearing at Pins  
4 and 5 of the LT6600-2.5 are the filter outputs. The  
Figure 2 shows how to AC couple signals into the  
LT6600-2.5. In this instance, the input is a single-ended  
signal. AC coupling allows the processing of single-ended  
or differential signals with arbitrary common mode levels.  
The 0.1µF coupling capacitor and the 1580gain setting  
resistor form a high pass filter, attenuating signals below  
1kHz. Larger values of coupling capacitors will propor-  
tionally reduce this highpass 3dB frequency.  
+
+
difference between VOUT and VOUT is the differential  
output voltage. The average of VOUT and VOUT is the  
common mode output voltage.  
Figure 1 illustrates the LT6600-2.5 operating with a single  
3.3V supply and unity passband gain; the input signal is  
DCcoupled. Thecommonmodeinputvoltageis0.5V, and  
the differential input voltage is 2VP-P. The common mode  
3.3V  
0.1µF  
V
V
3
1580Ω  
3
2
1
0
3
2
1
0
1
7
2
8
V
V
4
IN  
IN  
+
+
V
V
+
V
OUT  
OUT  
LT6600-2.5  
+
V
0.01µF  
1580Ω  
IN  
V
OUT  
+
OUT  
5
+
6
t
t
660025 F01  
V
IN  
Figure 1  
3.3V  
3
0.1µF  
V
V
0.1µF  
0.1µF  
1580Ω  
1580Ω  
1
7
2
3
2
1
0
2
1
4
+
+
V
V
+
OUT  
V
V
OUT  
LT6600-2.5  
+
V
IN  
0.01µF  
OUT  
0
t
8
OUT  
+
5
V
IN  
+
6
–1  
660025 F02  
Figure 2  
5V  
0.1µF  
V
V
3
402Ω  
1
+
3
3
V
4
IN  
+
+
V
V
OUT  
+
7
OUT  
LT6600-2.5  
2
1
0
2
1
2
8
V
OUT  
0.01µF  
402Ω  
V
500mV (DIFF)  
P-P  
OUT  
5
V
IN  
+
+
V
V
IN  
6
t
t
0
+
660025 F03  
2V  
IN  
Figure 3  
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LT6600-2.5  
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APPLICATIO S I FOR ATIO  
In Figure 3 the LT6600-2.5 is providing 12dB of gain. The  
common mode output voltage is set to 2V.  
Figure 5 is a laboratory setup that can be used to charac-  
terize the LT6600-2.5 using single-ended instruments  
with 50source impedance and 50input impedance.  
For a 12dB gain configuration the LT6600-2.5 requires a  
402sourceresistanceyetthenetworkanalyzeroutputis  
calibrated for a 50load resistance. The 1:1 transformer,  
53.6and 388resistors satisfy the two constraints  
above. The transformer converts the single-ended source  
into a differential stimulus. Similarly, the output of the  
LT6600-2.5 will have lower distortion with larger load  
resistance yet the analyzer input is typically 50. The 4:1  
turns (16:1 impedance) transformer and the two 402Ω  
resistors of Figure 5, present the output of the LT6600-2.5  
with a 1600differential load, or the equivalent of 800Ω  
to ground at each output. The impedance seen by the  
network analyzer input is still 50, reducing reflections in  
the cabling between the transformer and analyzer input.  
Use Figure 4 to determine the interface between the  
LT6600-2.5 and a current output DAC. The gain, or “trans-  
impedance,” is defined as A = VOUT/IIN. To compute the  
transimpedance, use the following equation:  
1580 R1  
A =  
( )  
R1+R2  
(
)
By setting R1 + R2 = 1580, the gain equation reduces to  
A = R1().  
The voltage at the pins of the DAC is determined by R1,  
R2, the voltage on Pin 7 and the DAC output current.  
Consider Figure 4 with R1 = 49.9and R2 = 1540. The  
voltage at Pin 7 is 1.65V. The voltage at the DAC pins is  
given by:  
Differential and Common Mode Voltage Ranges  
R1  
R1R2  
R1+R2  
V
DAC = VPIN7  
+I •  
IN  
Therail-to-railoutputstageoftheLT6600-2.5canprocess  
large differential signal levels. On a 3V supply, the output  
signal can be 5.1VP-P. Similarly, a 5V supply can support  
signals as large as 8.8VP-P. To prevent excessive power  
dissipation in the internal circuitry, the user must limit  
R1+R2 +1580  
= 26mV +I • 48.3Ω  
IN  
IIN is IIN+ or IIN. The transimpedance in this example is  
49.6.  
differential signal levels to 9VP-P  
.
Evaluating the LT6600-2.5  
The two amplifiers inside the LT6600-2.5 have indepen-  
dent control of their output common mode voltage (see  
the “Block Diagram” section). The following guidelines  
will optimize the performance of the filter.  
The low impedance levels and high frequency operation of  
the LT6600-2.5 require some attention to the matching  
networks between the LT6600-2.5 and other devices. The  
previous examples assume an ideal (0) source imped-  
ance and a large (1k) load resistance. Among practical  
examples where impedance must be considered is the  
evaluation of the LT6600-2.5 with a network analyzer.  
Pin 7 can be allowed to float; Pin 7 must be bypassed to an  
ACgroundwitha0.01µFcapacitororsomeinstabilitymay  
be observed. Pin 7 can be driven from a low impedance  
2.5V  
0.1µF  
CURRENT  
OUTPUT  
DAC  
3.3V  
COILCRAFT  
TTWB-16A  
4:1  
COILCRAFT  
TTWB-1010  
NETWORK  
ANALYZER  
SOURCE  
NETWORK  
ANALYZER  
INPUT  
0.1µF  
3
388Ω  
1:1  
1
7
2
8
402Ω  
4
+
3
R2  
R2  
I
I
IN  
1
7
2
8
50Ω  
LT6600-2.5  
4
+
53.6Ω  
50Ω  
V
V
+
OUT  
R1  
+
0.01µF  
LT6600-2.5  
5
+
402Ω  
388Ω  
6
IN  
OUT  
0.1µF  
5
+
660025 F05  
6
R1  
660025 F04  
2.5V  
Figure 5  
Figure 4  
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LT6600-2.5  
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APPLICATIO S I FOR ATIO  
source, provided it remains at least 1.5V above Vand at  
least 1.5V below V+. An internal resistor divider sets the  
voltage of Pin 7. While the internal 11k resistors are well  
matched, their absolute value can vary by ±20%. This  
should be taken into consideration when connecting an  
external resistor network to alter the voltage of Pin 7.  
amplifier inside the LT6600-2.5, and therefore sets the  
common mode output voltage of the filter. Since, in the  
example of Figure 3, Pin 2 differs from Pin 7 by 0.5V, an  
additional 625µA (312µA per side) of DC current will flow  
in the resistors coupling the 1st differential amplifier  
output stage to filter output. Thus, a total of 3.125mA is  
used to translate the common mode voltages.  
Pin 2 can be shorted to Pin 7 for simplicity. If a different  
common mode output voltage is required, connect Pin 2  
to a voltage source or resistor network. For 3V and 3.3V  
supplies the voltage at Pin 2 must be less than or equal to  
the mid supply level. For example, voltage (Pin 2) 1.65V  
on a single 3.3V supply. For power supply voltages higher  
than 3.3V the voltage at Pin 2 can be set above mid supply.  
The voltage on Pin 2 should not exceed 1V below the  
voltage on Pin 7. The voltage on Pin 2 should not be more  
than 2V above the voltage on Pin 7. Pin 2 is a high  
impedance input.  
A simple modification to Figure 3 will reduce the DC  
common mode currents by 36%. If Pin 7 is shorted to  
Pin 2 the common mode output voltage of both op amp  
stages will be 2V and the resulting DC current will be 2mA.  
Of course, by AC coupling the inputs of Figure 3, the  
common mode DC current can be reduced to 625µA.  
Noise  
The noise performance of the LT6600-2.5 can be evalu-  
ated with the circuit of Figure 6.  
TheLT6600-2.5wasdesignedtoprocessavarietyofinput  
signals including signals centered around the mid-supply  
voltage and signals that swing between ground and a  
positive voltage in a single supply system (Figure 1). The  
range of allowable input common mode voltage (the  
average of VIN and VIN in Figure 1) is determined by  
the power supply level and gain setting (see “Electrical  
Characteristics”).  
Given the low noise output of the LT6600-2.5 and the 6dB  
attenuation of the transformer coupling network, it will be  
necessary to measure the noise floor of the spectrum  
analyzer and subtract the instrument noise from the filter  
noise measurement.  
+
Example: With the IC removed and the 25resistors  
grounded, Figure 6, measure the total integrated noise  
(eS) of the spectrum analyzer from 10kHz to 2.5MHz. With  
the IC inserted, the signal source (VIN) disconnected, and  
the input resistors grounded, measure the total integrated  
noise out of the filter (eO). With the signal source con-  
nected, set the frequency to 100kHz and adjust the ampli-  
tude until VIN measures 100mVP-P. Measure the output  
amplitude, VOUT, and compute the passband gain  
Common Mode DC Currents  
In applications like Figure 1 and Figure 3 where the  
LT6600-2.5 not only provides lowpass filtering but also  
level shifts the common mode voltage of the input signal,  
DC currents will be generated through the DC path be-  
tweeninputandoutputterminals.Minimizethesecurrents  
to decrease power dissipation and distortion.  
2.5V  
0.1µF  
Consider the application in Figure 3. Pin 7 sets the output  
common mode voltage of the 1st differential amplifier  
inside the LT6600-2.5 (see the “Block Diagram” section)  
at 2.5V. Since the input common mode voltage is near 0V,  
there will be approximately a total of 2.5V drop across the  
series combination of the internal 1580feedback resis-  
tor and the external 402input resistor. The resulting  
1.25mA common mode DC current in each input path,  
must be absorbed by the sources VIN+ and VIN. Pin 2 sets  
the common mode output voltage of the 2nd differential  
SPECTRUM  
COILCRAFT  
ANALYZER  
R
R
3
TTWB-1010  
1:1  
IN  
IN  
V
IN  
INPUT  
1
7
2
8
25Ω  
4
+
LT6600-2.5  
50Ω  
5
+
25Ω  
0.1µF  
6
66002 F06  
2.5V  
Figure 6  
660025i  
8
LT6600-2.5  
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APPLICATIO S I FOR ATIO  
50  
40  
30  
20  
10  
0
100  
80  
A = VOUT/VIN. Now compute the input referred integrated  
noise (eIN) as:  
SPECTRAL DENSITY  
(eO)2 (eS)2  
60  
eIN =  
A
40  
Table 1 lists the typical input referred integrated noise for  
various values of RIN.  
20  
INTEGRATED  
Figure 7 is plot of the noise spectral density as a function  
of frequency for an LT6600-2.5 with RIN = 1580using  
the fixture of Figure 6 (the instrument noise has been  
subtracted from the results).  
0
0.01  
0.1  
1
10  
FREQUENCY (MHz)  
66002 F07  
Figure 7. Input Referred Noise, Gain = 1  
Table 1. Noise Performance  
INPUT REFERRED  
INTEGRATED NOISE INTEGRATED NOISE  
10kHz TO 2.5MHz 10kHz TO 5MHz  
INPUT REFERRED  
Table 2. LT6600-2.5 SO-8 Package Thermal Resistance  
COPPER AREA  
PASSBAND  
GAIN (V/V)  
R
IN  
TOPSIDE BACKSIDE BOARD AREA  
THERMAL RESISTANCE  
(JUNCTION-TO-AMBIENT)  
4
2
1
402Ω  
806Ω  
18µV  
29µV  
51µV  
23µV  
39µV  
73µV  
RMS  
RMS  
RMS  
RMS  
RMS  
RMS  
2
2
2
(mm )  
(mm )  
(mm )  
1100  
330  
35  
1100  
330  
35  
2500  
2500  
2500  
2500  
2500  
65°C/W  
1580Ω  
85°C/W  
95°C/W  
The noise at each output is comprised of a differential  
component and a common mode component. Using a  
transformerorcombinertoconvertthedifferentialoutputs  
tosingle-endedsignalrejectsthecommonmodenoiseand  
gives a true measure of the S/N achievable in the system.  
Conversely,ifeachoutputismeasuredindividuallyandthe  
noisepoweraddedtogether,theresultingcalculatednoise  
level will be higher than the true differential noise.  
35  
0
100°C/W  
0
0
105°C/W  
about 85°C/W. Without extra metal trace connected to the  
Vpin to provide a heat sink, the thermal resistance will be  
around 105°C/W. Table 2 can be used as a guide when  
considering thermal resistance.  
Junction temperature, TJ, is calculated from the ambient  
temperature, TA, and power dissipation, PD. The power  
dissipation is the product of supply voltage, VS, and  
supply current, IS. Therefore, the junction temperature is  
given by:  
Power Dissipation  
TheLT6600-2.5amplifierscombinehighspeedwithlarge-  
signal currents in a small package. There is a need to  
ensure that the dies’s junction temperature does not  
exceed150°C. TheLT6600-2.5packagehasPin6fusedto  
the lead frame to enhance thermal conduction when  
connecting to a ground plane or a large metal trace. Metal  
trace and plated through-holes can be used to spread the  
heat generated by the device to the backside of the PC  
board. For example, on a 3/32" FR-4 board with 2oz  
copper, a total of 660 square millimeters connected to Pin  
6 of the LT6600-2.5 (330 square millimeters on each side  
of the PC board) will result in a thermal resistance, θJA, of  
TJ = TA + (PD θJA) = TA + (VS • IS θJA)  
where the supply current, IS, is a function of signal level,  
load impedance, temperature and common mode  
voltages.  
For a given supply voltage, the worst-case power dissi-  
pation occurs when the differential input signal is maxi-  
mum, the common mode currents are maximum (see  
Applications Information regarding Common Mode DC  
660025i  
9
LT6600-2.5  
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APPLICATIO S I FOR ATIO  
Currents), the load impedance is small and the ambient  
temperature is maximum. To compute the junction tem-  
perature, measure the supply current under these worst-  
case conditions, estimate the thermal resistance from  
Table2, thenapplytheequationforTJ. Forexample, using  
the circuit in Figure 3 with DC differential input voltage of  
1V, a differential output voltage of 4V, no load resistance  
and an ambient temperature of 85°C, the supply current  
(current into Pin 3) measures 37.6mA. Assuming a PC  
board layout with a 35mm2 copper trace, the θJA is  
100°C/W. The resulting junction temperature is:  
TJ = TA + (PD θJA) = 85 + (5 • 0.0376 • 100) = 104°C  
When using higher supply voltages or when driving small  
impedances, more copper may be necessary to keep TJ  
below 150°C.  
660025i  
10  
LT6600-2.5  
U
PACKAGE DESCRIPTIO  
S8 Package  
8-Lead Plastic Small Outline (Narrow .150 Inch)  
(Reference LTC DWG # 05-08-1610)  
.189 – .197  
(4.801 – 5.004)  
.045 ±.005  
NOTE 3  
.050 BSC  
7
5
8
6
.245  
MIN  
.160 ±.005  
.150 – .157  
(3.810 – 3.988)  
NOTE 3  
.228 – .244  
(5.791 – 6.197)  
.030 ±.005  
TYP  
1
3
4
2
RECOMMENDED SOLDER PAD LAYOUT  
.010 – .020  
(0.254 – 0.508)  
× 45°  
.053 – .069  
(1.346 – 1.752)  
.004 – .010  
(0.101 – 0.254)  
.008 – .010  
(0.203 – 0.254)  
0°– 8° TYP  
.016 – .050  
(0.406 – 1.270)  
.050  
(1.270)  
BSC  
.014 – .019  
(0.355 – 0.483)  
TYP  
NOTE:  
INCHES  
1. DIMENSIONS IN  
(MILLIMETERS)  
2. DRAWING NOT TO SCALE  
3. THESE DIMENSIONS DO NOT INCLUDE MOLD FLASH OR PROTRUSIONS.  
MOLD FLASH OR PROTRUSIONS SHALL NOT EXCEED .006" (0.15mm)  
SO8 0303  
660025i  
11  
LT6600-2.5  
RELATED PARTS  
PART NUMBER  
LTC®1565-31  
LTC1566-1  
LT1567  
DESCRIPTION  
COMMENTS  
650kHz Linear Phase Lowpass Filter  
Continuous Time, SO8 Package, Fully Differential  
Continuous Time, SO8 Package  
Low Noise, 2.3MHz Lowpass Filter  
Very Low Noise, High Frequency Filter Building Block  
Very Low Noise, 4th Order Building Block  
1.4nV/Hz Op Amp, MSOP Package, Fully Differential  
LT1568  
Lowpass and Bandpass Filter Designs Up to 10MHz,  
Differential Outputs  
LT6600-10  
LT6600-20  
Very Low Noise Differential Amplifier and 10MHz  
Lowpass Filter  
82dB S/N with 3V Supply, SO-8 Package  
Very Low Noise Differential Amplifier and 20MHz  
Lowpass Filter  
76dB S/N with 3V Supply, SO-8 Package  
660025i  
LT/TP 0603 1K • PRINTED IN USA  
12 LinearTechnology Corporation  
1630 McCarthy Blvd., Milpitas, CA 95035-7417  
(408) 432-1900 FAX: (408) 434-0507 www.linear.com  
LINEAR TECHNOLOGY CORPORATION 2003  

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