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參數資料
| 型號： | MC88PL117FN |
| 廠商： | MOTOROLA INC |
| 元件分類： | 時鐘及定時 |
| 英文描述： | CMOS PLL CLOCK DRIVER |
| 中文描述： | 88PL SERIES, PLL BASED CLOCK DRIVER, 15 TRUE OUTPUT(S), 0 INVERTED OUTPUT(S), PQCC52 |
| 封裝： | PLASTIC, LCC-52 |
| 文件頁數： | 10/11頁 |
| 文件大小： | 139K |
| 代理商： | MC88PL117FN |
MC88PL117
MOTOROLA
TIMING SOLUTIONS
BR1333 — Rev 6
10
OUTLINE DIMENSIONS
FN SUFFIX
PLASTIC PACKAGE
CASE 778-02
ISSUE C
–L–
Y
BRK
W
D
D
V
52
1
NOTES:
1. DATUMS –L–, –M–, AND –N– DETERMINED WHERE
TOP OF LEAD SHOULDER EXITS PLASTIC BODY AT
MOLD PARTING LINE.
2. DIMENSION G1, TRUE POSITION TO BE MEASURED
AT DATUM –T–, SEATING PLANE.
3. DIMENSIONS R AND U DO NOT INCLUDE MOLD
FLASH. ALLOWABLE MOLD FLASH IS 0.010 (0.250)
PER SIDE.
4. DIMENSIONING AND TOLERANCING PER ANSI
Y14.5M, 1982.
5. CONTROLLING DIMENSION: INCH.
6. THE PACKAGE TOP MAY BE SMALLER THAN THE
PACKAGE BOTTOM BY UP TO 0.012 (0.300).
DIMENSIONS R AND U ARE DETERMINED AT THE
OUTERMOST EXTREMES OF THE PLASTIC BODY
EXCLUSIVE OF MOLD FLASH, TIE BAR BURRS, GATE
BURRS AND INTERLEAD FLASH, BUT INCLUDING
ANY MISMATCH BETWEEN THE TOP AND BOTTOM
OF THE PLASTIC BODY.
7. DIMENSION H DOES NOT INCLUDE DAMBAR
PROTRUSION OR INTRUSION. THE DAMBAR
PROTRUSION(S) SHALL NOT CAUSE THE H
DIMENSION TO BE GREATER THAN 0.037 (0.940).
THE DAMBAR INTRUSION(S) SHALL NOT CAUSE THE
H DIMENSION TO BE SMALLER THAN 0.025 (0.635).
B
U
Z
G1
X
VIEW D–D
H
K1
K
F
VIEW S
M
0.007 (0.18)
L–M
S
T
S
N
M
0.007 (0.18)
L–M
S
T
S
N
0.004 (0.100)
–T–
SEATING
M
0.007 (0.18)
L–M
S
T
S
N
M
0.007 (0.18)
L–M
S
T
S
N
A
R
G
G1
C
Z
J
E
VIEW S
–M–
–N–
DIM
A
B
C
E
F
G
H
J
K
R
U
V
W
X
Y
Z
G1
K1
MIN
0.785
0.785
0.165
0.090
0.013
0.050 BSC
0.026
0.020
0.025
0.750
0.750
0.042
0.042
0.042
–––
2
0.710
0.040
MAX
0.795
0.795
0.180
0.110
0.019
MIN
19.94
19.94
4.20
2.29
0.33
MAX
20.19
20.19
4.57
2.79
0.48
MILLIMETERS
INCHES
1.27 BSC
0.66
0.51
0.64
19.05
19.05
1.07
1.07
1.07
–––
2
18.04
1.02
0.032
–––
–––
0.756
0.756
0.048
0.048
0.056
0.020
10
0.730
–––
0.81
–––
–––
19.20
19.20
1.21
1.21
1.42
0.50
10
18.54
–––
M
0.007 (0.18)
L–M
S
T
S
N
M
0.007 (0.18)
L–M
S
T
S
N
S
0.010 (0.25)
L–M
S
T
S
N
S
0.010 (0.25)
L–M
S
T
S
N
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