10
FN7384.7
January 16, 2008
FIGURE 33. EL5150 ENABLE/DISABLE FIGURE 34. EL5250 ENABLE/DISABLE
FIGURE 35. DIFFERENTIAL GAIN FIGURE 36. DIFFERENTIAL PHASE
FIGURE 37. SMALL SIGNAL FREQUENCY vs SUPPLY FIGURE 38. INPUT-TO-OUTPUT ISOLATION WITH PART
DISABLED
Typical Performance Curves (Continued)
TIME (400ns/DIV)
CH 1
CH 4
210ns
ENABLE
620ns
DISABLE
A
V
= +1
R
L
= 500Ω
R
L
= 500Ω
SUPPLY = ±5.0V, ±2.7mA
800ns
ENABLE
520ns
DISABLE
TIME (1µs/DIV)
CH 2
0 10010 80
-0.04
DIFFERENTIAL
GAIN (%)
-0.02
4020 5030
0
60 70
0.02
0.04
0.06
90
IRE
010010 80
-1.0
DIFFERENTIAL
PHASE (°)
IRE
-0.5
4020 5030
0
60 70
0.5
1.0
1.5
90
A
V
= +1
R
L
= 500Ω
C
L
= 5pF
100k 300M10M
4
2
-2
-6
NORMALIZED GAIN (dB)
FREQUENCY (Hz)
-4
100M1M
0
±2.0V
±6.0V
A
V
= +1
R
L
= 500Ω
C
L
= 2.7pF
100k 300M10M
-50
-70
-110
-150
ISOSLATION (dB)
FREQUENCY (Hz)
-130
100M1M
-90
EL5150, EL5151, EL5250, EL5251, EL5451
11
FN7384.7
January 16, 2008
Product Description
The EL5150, EL5151, EL5250, EL5251 and EL5451 are
wide bandwidth, low power, low offset voltage feedback
operational amplifiers capable of operating from a single or
dual power supplies. This family of operational amplifiers are
internally compensated for closed loop gain of +1 or greater.
Connected in voltage follower mode, driving a 500Ω load
members of this amplifier family demonstrate a -3dB
bandwidth of about 200MHz. With the loading set to
accommodate typical video application, 150Ω load and gain
set to +2, bandwidth reduces to about 40MHz with a 67V/µs
slew rate. Power down pins on the EL5151 and EL5251
reduce the already low power demands of this amplifier
family to 12µA typical while the amplifier is disabled.
Input, Output and Supply Voltage Range
The EL5150 and family members have been designed to
operate with supply voltage ranging from 5V to 12V. Supply
voltages range from ±2.5V to ±5V for split supply operation.
And of course split supply operation can easily be achieved
using single supplies with by splitting off half of the single
supply with a simple voltage divider as illustrated in the
application circuit section.
Input Common Mode Range
These amplifiers have an input common mode voltage
ranging from 3.5V above the negative supply (V
S
- pin) to
3.5V below the positive supply (V
S
+ pin). If the input signal is
driven beyond this range the output signal will exhibit
distortion.
Maximum Output Swing & Load Resistance
The outputs of the EL5150 and family members exhibit
maximum output swing ranges from -4V to 4V for V
S
= ±5V
with a load resistance of 500Ω. Naturally, as the load
resistance becomes lower, the output swing lowers
accordingly; for instance, if the load resistor is 150Ω, the
output swing ranges from -3.5V to 3.5V. This response is a
simple application of Ohms law indicating a lower value
resistance results in greater current demands of the
amplifier. Additionally, the load resistance affects the
frequency response of this family as well as all operational
amplifiers; as clearly indicated by the Gain vs Frequency For
Various R
L
curves clearly indicate. In the case of the
frequency response reduced bandwidth with decreasing
load resistance is a function of load resistance in conjunction
with the output zero response of the amplifier.
Choosing A Feedback Resistor
A feedback resistor is required to achieve unity gain; simply
short the output pin to the inverting input pin. Gains greater
than +1 require a feedback and gain resistor to set the
desired gain. This gets interesting because the feedback
resistor forms a pole with the parasitic capacitance at the
inverting input; as the feedback resistance increases the
position of the pole shifts in the frequency domain, the
amplifier's phase margin is reduced and the amplifier
becomes less stable. Peaking in the frequency domain and
ringing in the time domain are symptomatic of this shift in
pole location. So we want to keep the feedback resistor as
small as possible. You may want to use a large feedback
resistor for some reason; in this case to compensate the shift
of the pole and maintain stability a small capacitor in the few
Pico farad range in parallel with the feedback resistor is
recommended.
For the gains greater than unity it has been determined a
feedback resistance ranging from 500Ω to 750Ω provides
optimal response.
FIGURE 39. PACKAGE POWER DISSIPATION vs AMBIENT
TEMPERATURE
FIGURE 40. PACKAGE POWER DISSIPATION vs AMBIENT
TEMPERATURE
Typical Performance Curves (Continued)
JEDEC JESD51-7 HIGH EFFECTIVE THERMAL
CONDUCTIVITY TEST BOARD
1.136W
909mW
870mW
435mW
0 15050
1.4
1.2
0.4
0
POWER DISSPIATION (W)
AMBIENT TEMPERATURE (°C)
0.2
12525
0.8
10075 85
1.0
0.6
θ
JA
= 88°C/W
SO14
θ
JA
= 230°C/W
SOT23-5/6
θ
JA
= 110°C/W
SO8
θ
JA
= 115°C/W
MSOP8/10
JEDEC JESD51-3 LOW EFFECTIVE THERMAL
CONDUCTIVITY TEST BOARD
0 15050
1
0.9
0.2
0
POWER DISSPIATION (W)
AMBIENT TEMPERATURE (°C)
0.1
12525
0.5
10075 85
0.7
0.3
0.8
0.4
0.6
833mW
625mW
486mW
391mW
θ
JA
= 265°C/W
SOT23-5/6
θ
JA
= 206°C/W
MSOP8/10
θ
JA
= 120°C/W
SO14
θ
JA
= 160°C/W
SO8
EL5150, EL5151, EL5250, EL5251, EL5451
12
FN7384.7
January 16, 2008
Gain Bandwidth Product
The EL5150 and family members have a gain bandwidth
product of 40MHz for a gain of +5. Bandwidth can be
predicted by the following equation:
(Gain) x (BW) = GainBandwidthProduct
Video Performance
For good video performance, an amplifier is required to
maintain the same output impedance and same frequency
response as DC levels are changed at the output; this
characteristic is widely referred to as “diffgain-diffphase”.
Many amplifiers have a difficult time with this especially while
driving standard video loads of 150Ω, as the output current
has a natural tendency to change with DC level. The dG and
dP for these families is a respectable 0.04% and 0.9°, while
driving 150Ω at a gain of 2. Driving high impedance loads
would give a similar or better dG and dP performance as the
current output demands placed on the amplifier lessen with
increased load.
Driving Capacitive Loads
These devices can easily drive capacitive loads as
demanding as 27pF in parallel with 500Ω while holding
peaking to within 5dB of peaking at unity gain. Of course if
less peaking is desired, a small series resistor (usually
between 5Ω to 50Ω) can be placed in series with the output
to eliminate most peaking; however, there will be a small
sacrifice of gain which can be recovered by simply adjusting
the value of the gain resistor.
Driving Cables
Both ends of all cables must always be properly terminated;
double termination is absolutely necessary for reflection-free
performance. Additionally, a back-termination series resistor
at the amplifier's output will isolate the amplifier from the
cable and allow extensive capacitive drive. However, other
applications may have high capacitive loads without a
back-termination resistor. Again, a small series resistor at
the output can help to reduce peaking.
Disable/Power-Down
Devices with disable can be disabled with their output placed
in a high impedance state. The turn off time is about 330ns
and the turn on time is about 130ns. When disabled, the
amplifier's supply current is reduced to 17µA typically;
essentially eliminating power consumption. The amplifier's
power down is controlled by standard TTL or CMOS signal
levels at the ENABLE pin. The applied logic signal is relative
to V
S
- pin. Letting the ENABLE pin float or the application of
a signal that is less than 0.8V above V
S
- enables the
amplifier. The amplifier is disabled when the signal at
ENABLE pin is above V
S
+ - 1.5V.
Output Drive Capability
Members of the EL5150 family do not have internal short
circuit protection circuitry. Typically, short circuit currents
ranging from 70mA and 95mA can be expected and
naturally, if the output is shorted indefinitely the part can
easily be damaged from overheating; or excessive current
density may eventually compromise metal integrity.
Maximum reliability is maintained if the output current is
always held below ±40mA. This limit is set and limited by the
design of the internal metal interconnect. Note that in
transient applications, the part is extremely robust.
Power Dissipation
With the high output drive capability of these devices, it is
possible to exceed the +125°C absolute maximum junction
temperature under certain load current conditions.
Therefore, it is important to calculate the maximum junction
temperature for an application to determine if load conditions
or package types need to be modified to assure operation of
the amplifier in a safe operating area.
The maximum power dissipation allowed in a package is
determined according to Equation 1:
Where:
T
JMAX
= Maximum junction temperature
T
AMAX
= Maximum ambient temperature
θ
JA
= Thermal resistance of the package
The maximum power dissipation actually produced by an IC
is the total quiescent supply current times the total power
supply voltage, plus the power in the IC due to the load, or:
For sourcing:
For sinking:
Where:
V
S
= Supply voltage
I
SMAX
= Maximum quiescent supply current
V
OUT
= Maximum output voltage of the application
R
LOAD
= Load resistance tied to ground
I
LOAD
= Load current
N = number of amplifiers (Max = 2)
By setting the two PD
MAX
equations equal to each other, we
can solve the output current and R
LOAD
to avoid the device
overheat.
PD
MAX
T
JMAX
T
AMAX
Θ
JA
---------------------------------------------
=
(EQ. 1)
PD
MAX
V
S
I
SMAX
V
S
V
OUTi
()
i1=
n
V
OUTi
R
Li
-----------------
×+×=
(EQ. 2)
PD
MAX
V
S
I
SMAX
V
OUTi
V
S
()
i1=
n
I
LOADi
×+×=
(EQ. 3)
EL5150, EL5151, EL5250, EL5251, EL5451

EL5151IWZ-T7

Mfr. #:
Manufacturer:
Renesas / Intersil
Description:
IC OPAMP VFB 1 CIRCUIT SOT23-5
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
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