the ambient temperature TA
參數資料
型號: LT1994CDD#TRPBF
廠商: Linear Technology
文件頁數: 7/20頁
文件大?。?/td> 0K
描述: IC DIFF AMP/DRIVER LN 8-DFN
標準包裝: 2,500
放大器類型: 差分
電路數: 1
輸出類型: 滿擺幅
轉換速率: 65 V/µs
增益帶寬積: 70MHz
電流 - 輸入偏壓: 18µA
電壓 - 輸入偏移: 3000µV
電流 - 電源: 14.8mA
電流 - 輸出 / 通道: 85mA
電壓 - 電源,單路/雙路(±): 2.375 V ~ 12.6 V,±1.188 V ~ 6.3 V
工作溫度: 0°C ~ 70°C
安裝類型: 表面貼裝
封裝/外殼: 8-WFDFN 裸露焊盤
供應商設備封裝: 8-DFN-EP(3x3)
包裝: 帶卷 (TR)
15
1994fb
LT1994
In general, the die temperature can be estimated from
the ambient temperature TA, and the device power dis-
sipation PD:
TJ = TA+ + PD θJA
The power dissipation in the IC is a function of the supply
voltage, the output voltage, and the load resistance. For
fully differential output ampliers at a given supply voltage
(±VCC), and a given differential load (RLOAD), the worst-
case power dissipation PD(MAX) occurs at the worst-case
quiescent current (IQ(MAX) = 20.5mA) and when the load
current is given by the expression:
I
V
R
LOAD
CC
LOAD
=
The worst-case power dissipation in the LT1994 at
I
V
R
LOAD
CC
LOAD
=
is:
PV
I
R
V
R
VI
DMAX
CC
LOAD
Q MAX
LOAD
CC
LOAD
CC
QMAX
()
=+
()
=+
2
Example: A LT1994 is mounted on a circuit board in a
MSOP-8 package (
θJA = 140°C/W), and is running off of
±5V supplies driving an equivalent load (external load plus
feedback network) of 75
Ω. The worst-case power that
would be dissipated in the device occurs when:
P
V
R
VI
V
DMAX
CC
LOAD
CC
QMAX
()
=+
2
5
75
25
Ω
.
17 5
0 54
MA
W
=
The maximum ambient temperature the 8-lead MSOP is
allowed to operate under these conditions is:
TA = TJMAX – PD θJA = 150°C – (0.54W)
(140°C/W) = 75°C
To operate the device at higher ambient temperature,
connect more copper to the Vpin to reduce the thermal
resistance of the package as indicated in Table 1.
Table 1. LT1994 MSOP Package Thermal Resistivity
COPPER AREA
TOPSIDE (mm2)
COPPER AREA
BACKSIDE (mm2)
THERMAL RESISTANCE
(JUNCTION-TO-AMBIENT)
00
140
30
0
135
100
0
130
100
120
540
110
Layout Considerations
Because the LT1994 is a high speed amplier, it is sensitive
to both stray capacitance and stray inductance. Compo-
nents connected to the LT1994 should be connected with
as short and direct connections as possible. A low noise,
low impedance ground plane is critical for the highest
performance. In single-supply applications, high quality
surface mount 1μF and 0.1μF ceramic bypass capacitors
with minimum PCB trace should be used directly across
the power supplies V+ to V. In split supply applications,
high quality surface mount 1μF and 0.1μF ceramic bypass
capacitors should be placed across the power supplies
V+ to V, and individual high quality surface mount 0.1μF
bypass capacitors should be used from each supply to
ground with direct (short) connections.
Any stray parasitic capacitance to ground at the summing
junctions, IN+ and INshould be kept to an absolute mini-
mum even if it means stripping back the ground plane
away from any trace attached to this node. This becomes
especially true when the feedback resistor network uses
resistor values >500
Ω in circuits with RF = RI. Excessive
peaking in the frequency response can be mitigated by
adding small amounts of feedback capacitance around RF
(2pF to 5pF). Always keep in mind the differential nature of
the LT1994, and that it is critical that the output impedances
seen by both outputs (stray or intended) should be as bal-
anced and symmetric as possible. This will help preserve
the natural balance of the LT1994, which minimizes the
generation of even order harmonics, and preserves the
rejection of common mode signals and noise.
It is highly recommended that the VOCM pin be either hard
tied to a low impedance ground plane (in split supply
applications) or bypassed to ground with a high quality
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