LT1507 Linear Technology, LT1507 Datasheet - Page 18
LT1507
Manufacturer Part Number
LT1507
Description
500kHz Monolithic Buck Mode Switching Regulator
Manufacturer
Linear Technology
Datasheet
1.LT1507.pdf
(20 pages)
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
Part Number:
LT15073
Manufacturer:
LT/凌特
Quantity:
20 000
Part Number:
LT15073CS8
Manufacturer:
LT/凌特
Quantity:
20 000
Part Number:
LT1507CN8#PBF
Manufacturer:
LINEAR/凌特
Quantity:
20 000
Part Number:
LT1507CS8
Manufacturer:
LT
Quantity:
20 000
Part Number:
LT1507CS8#PBF
Manufacturer:
LINEAR/凌特
Quantity:
20 000
Company:
Part Number:
LT1507CS8#TR
Manufacturer:
SEOUL
Quantity:
3 223
Company:
Part Number:
LT1507CS8-3.3
Manufacturer:
LT
Quantity:
10 000
LT1507
APPLICATIONS
Example: with V
Total power dissipation is 0.3 + 0.046 + 0.032 = 0.38W.
Thermal resistance for the LT1507 packages is influenced
by the presence of internal or backside planes. With a full
plane under the SO package, thermal resistance will be
about 120 C/W. No plane will increase resistance to about
150 C/W. To calculate die temperature, use the proper
thermal resistance number for the desired package and
add in worst-case ambient temperature;
With the S8 package (
temperature of 70 C;
FREQUENCY COMPENSATION
The LT1507 uses a “current mode” architecture to help
alleviate phase shift created by the inductor. The basic
connections are shown in Figure 9. Gain of the power stage
can be modeled as 1.8A/V transconductance from the V
pin voltage to current delivered to the output. This is
shown in Figure 8 where the transconductance from V
pin to inductor current is essentially flat from 50Hz to
50kHz and phase shift is minimal in the important loop
unity-gain band of 1kHz to 50kHz. Inductor variation from
3 H to 20 H will have very little effect on these curves.
Overall gain from the V
the product of 1.8A/V transconductance multiplied by the
complex impedance of the load in parallel with the output
capacitor model.
The error amplifier can be modeled as a transconductance
of 2000 mho, with an output impedance of 200k
18
T
T
P
P
P
SW
Q
J
J
BOOST
= T
= 70 + 120(0.38) = 116 C
5 0 003
A
( .
( . )( ) ( . )
0 26 0 04 0 3
+
0 4 1 3 3
.
( . )
JA
3 3
(P
5
IN
5
)
2
TOT
2
= 5V, V
.
U
3 3 0 005
0 008
. ( .
)
.
C
pin to output is then modeled as
INFORMATION
JA
OUT
U
.
16 10
W
= 120 C/W) at an ambient
)
75
= 3.3V, I
1
0 032
.
9
W
0 046
.
OUT
1 5 500 10
W
W
= 1A;
U
3
in
C
C
parallel with 12pF. In all practical applications, the com-
pensation network from V
lower impedance than the output impedance of the ampli-
fier at frequencies above 500Hz. This means that the error
amplifier characteristics themselves do not contribute
excess phase shift to the loop and the phase/gain charac-
teristics of the error amplifier section are completely
controlled by the external compensation network.
The complete small-signal model is shown in Figure 9. R1
and R2 are the divider used to set output voltage. These are
internal on the fixed voltage LT1507-3.3 with R1 = 1.8k
and R2 = 5k. R
GND
Figure 9. Small-Signal Model for Loop Stability Analysis
12pF
200k
POWER STAGE
g
C
m
Figure 8. Phase and Gain from V
to Inductor Current
F
= 1.8A/V
2.0
1.5
1.0
0.5
0
R
ERROR AMPLIFIER
g
10
V
C
m
C
C
C
V
I
V
L = 10 H
= 2000 ho
OUT
OUT
IN
C
= 5V
, C
= 250mA
= 3.3V
100
C
and C
–
+
FREQUENCY (Hz)
LT1507
PHASE
2.42V
GAIN (A/V)
1k
C
F
pin to ground has a much
are external compensation
V
F
SW
B
10k
C
L1
LT1507 • F08
Pin Voltage
100k
R1
R2
80
40
0
–40
–80
1507 • F09
+
ESR
OUTPUT
C1