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LT1795
(Rev.:RevA)

Dual 500mA/50MHz Current Feedback Line Driver Amplifier

Linear Technology 

LT1795

APPLICATIO S I FOR ATIO

ture until the device begins thermal shutdown gives a

good indication of how much margin there is in the

thermal design.

For surface mount devices, heat sinking is accomplished

by using the heat spreading capabilities of the PC board

and its copper traces. For the TSSOP package, power is

dissipated through the exposed heatsink. For the SO

package, power is dissipated from the package primarily

through the V – pins (4 to 7 and 14 to 17). These pins

should have a good thermal connection to a copper plane,

either by direct contact or by plated through holes. The

copper plane may be an internal or external layer. The

thermal resistance, junction-to-ambient will depend on

the total copper area connected to the device. For example,

the thermal resistance of the LT1795 connected to a 2 × 2

inch, double sided 2 oz copper plane is 40°C/W.

ing 0.5A current peaks into the load, a 1Ω power supply

impedance will cause a droop of 0.5V, reducing the

available output swing by that amount. Surface mount

tantalum and ceramic capacitors make excellent low ESR

bypass elements when placed close to the chip. For

frequencies above 100kHz, use 1µF and 100nF ceramic

capacitors. If significant power must be delivered below

100kHz, capacitive reactance becomes the limiting factor.

Larger ceramic or tantalum capacitors, such as 4.7µF, are

recommended in place of the 1µF unit mentioned above.

Inadequate bypassing is evidenced by reduced output

swing and “distorted” clipping effects when the output is

driven to the rails. If this is observed, check the supply pins

of the device for ripple directly related to the output

waveform. Significant supply modulation indicates poor

bypassing.

CALCULATING JUNCTION TEMPERATURE

The junction temperature can be calculated from the

equation:

TJ = (PD)(θJA) + TA

where

TJ = Junction Temperature

TA = Ambient Temperature

PD = Device Dissipation

θJA = Thermal Resistance (Junction-to-Ambient)

Differential Input Signal Swing

The differential input swing is limited to about ±5V by an

ESD protection device connected between the inputs. In

normal operation, the differential voltage between the

input pins is small, so this clamp has no effect. However,

in the shutdown mode, the differential swing can be the

same as the input swing. The clamp voltage will then set

the maximum allowable input voltage.

POWER SUPPLY BYPASSING

To obtain the maximum output and the minimum distor-

tion from the LT1795, the power supply rails should be

well bypassed. For example, with the output stage supply-

Capacitance on the Inverting Input

Current feedback amplifiers require resistive feedback

from the output to the inverting input for stable operation.

Take care to minimize the stray capacitance between the

output and the inverting input. Capacitance on the invert-

ing input to ground will cause peaking in the frequency

response (and overshoot in the transient response), but it

does not degrade the stability of the amplifier.

Feedback Resistor Selection

The optimum value for the feedback resistors is a function

of the operating conditions of the device, the load imped-

ance and the desired flatness of response. The Typical AC

Performance tables give the values which result in less

than 1dB of peaking for various resistive loads and oper-

ating conditions. If this level of flatness is not required, a

higher bandwidth can be obtained by use of a lower

feedback resistor.

For resistive loads, the COMP pin should be left open (see

Capacitive Loads section).

Capacitive Loads

The LT1795 includes an optional compensation network

for driving capacitive loads. This network eliminates most

of the output stage peaking associated with capacitive

loads, allowing the frequency response to be flattened.

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