MC10H641FN

更新时间:2024-09-18 02:28:38
品牌:MOTOROLA
描述:SINGLE SUPPLY PECL-TTL 1:9 CLOCK DISTRIBUTION CHIP

MC10H641FN 概述

SINGLE SUPPLY PECL-TTL 1:9 CLOCK DISTRIBUTION CHIP 单电源PECL - TTL 1 : 9时钟分配芯片 时钟驱动器

MC10H641FN 规格参数

生命周期:Transferred零件包装代码:QLCC
包装说明:QCCJ, LDCC28,.5SQ针数:28
Reach Compliance Code:unknownHTS代码:8542.39.00.01
风险等级:5.35Is Samacsys:N
其他特性:PECL-TTL CLOCK DISTRIBUTOR系列:10H
输入调节:DIFFERENTIAL LATCHEDJESD-30 代码:S-PQCC-J28
JESD-609代码:e0长度:11.5062 mm
负载电容(CL):50 pF逻辑集成电路类型:LOW SKEW CLOCK DRIVER
最大I(ol):0.024 A功能数量:1
反相输出次数:端子数量:28
实输出次数:9最高工作温度:85 °C
最低工作温度:封装主体材料:PLASTIC/EPOXY
封装代码:QCCJ封装等效代码:LDCC28,.5SQ
封装形状:SQUARE封装形式:CHIP CARRIER
电源:5 V最大电源电流(ICC):65 mA
Prop。Delay @ Nom-Sup:6.4 ns认证状态:Not Qualified
Same Edge Skew-Max(tskwd):0.35 ns座面最大高度:4.57 mm
子类别:Clock Drivers最大供电电压 (Vsup):5.25 V
最小供电电压 (Vsup):4.75 V标称供电电压 (Vsup):5 V
表面贴装:YES技术:ECL
温度等级:OTHER端子面层:Tin/Lead (Sn/Pb)
端子形式:J BEND端子节距:1.27 mm
端子位置:QUAD宽度:11.5062 mm
Base Number Matches:1

MC10H641FN 数据手册

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SEMICONDUCTOR TECHNICAL DATA  
The MC10H/100H641 is a single supply, low skew translating 1:9 clock  
driver. Devices in the Motorola H600 translator series utilize the 28–lead  
PLCC for optimal power pinning, signal flow through and electrical  
performance.  
SINGLE SUPPLY  
PECL–TTL 1:9 CLOCK  
DISTRIBUTION CHIP  
The device features a 24mA TTL output stage, with AC performance  
specified into a 50pF load capacitance. A latch is provided on–chip. When  
LEN is LOW (or left open, in which case it is pulled LOW by the internal  
pulldown) the latch is transparent. A HIGH on the enable pin (EN) forces  
all outputs LOW. Both the LEN and EN pins are positive ECL inputs.  
The V  
output is provided in case the user wants to drive the device  
with a single–ended input. For single–ended use the V should be  
BB  
BB  
connected to the D input and bypassed with a 0.01µF capacitor.  
The 10H version of the H641 is compatible with positive MECL 10H  
logic levels. The 100H version is compatible with positive 100K levels.  
PECL–TTL Version of Popular ECLinPS E111  
Low Skew  
Guaranteed Skew Spec  
Latched Input  
Differential ECL Internal Design  
FN SUFFIX  
PLASTIC PACKAGE  
CASE 776–02  
V  
Output for Single–Ended Use  
BB  
Single +5V Supply  
Logic Enable  
Extra Power and Ground Supplies  
Separate ECL and TTL Supply Pins  
Pinout: 28–Lead PLCC (Top View)  
GT  
Q6  
VT  
Q7  
VT  
Q8  
GT  
PIN NAMES  
25  
24  
23  
22  
21  
20  
19  
Pins  
Function  
GT  
Q5  
VT  
Q4  
VT  
Q3  
GT  
26  
27  
28  
18  
17  
16  
15  
14  
13  
12  
VBB  
D
GT, VT  
GE, VE  
D, D  
TTL GND, TTL V  
CC  
ECL GND, ECL V  
CC  
Signal Input (Positive ECL)  
V Reference Output  
D
V
BB  
BB  
(Positive ECL)  
VE  
LEN  
GE  
EN  
1
2
Q0–Q8  
EN  
LEN  
Signal Outputs (TTL)  
Enable Input (Positive ECL)  
Latch Enable Input  
(Positive ECL)  
3
4
5
6
7
8
9
10  
11  
GT  
Q2  
VT  
Q1  
VT  
Q0  
GT  
MECL 10H is a trademark of Motorola, Inc.  
11/93  
REV 3  
Motorola, Inc. 1996  
MC10H641 MC100H641  
LOGIC DIAGRAM  
TTL Outputs  
Q0  
Q1  
Q2  
Q3  
Q4  
Q5  
Q6  
Q7  
Q8  
PECL Input  
D
D
D
Q
VBB  
LEN  
EN  
DC CHARACTERISTICS (VT = VE = 5.0V ±5%)  
T
A
= 0°C  
T
A
= + 25°C  
T
A
= + 85°C  
Typ  
Symbol  
Characteristic  
Min  
Typ  
Max  
Min  
Typ  
Max  
Min  
Max  
Unit  
Condition  
I
Power Supply Current  
PECL  
24  
30  
24  
30  
24  
30  
mA  
EE  
I
I
TTL  
24  
27  
30  
35  
24  
27  
30  
35  
24  
27  
30  
35  
mA  
mA  
CCH  
CCL  
TTL DC CHARACTERISTICS (VT = VE = 5.0V ±5%)  
0°C  
25°C  
85°C  
Symbol  
Characteristic  
Output HIGH Voltage  
Min  
Max  
Min  
2.5  
Max  
Min  
Max  
Unit  
V
Condition  
V
V
2.5  
2.5  
I
I
= –15mA  
= 24mA  
OH  
OH  
Output LOW Voltage  
0.5  
0.5  
0.5  
V
OL  
OL  
I
Output Short Circuit Current  
–100  
–225  
–100  
–225  
–100  
–225  
mA  
V
OUT  
= 0V  
OS  
10H PECL DC CHARACTERISTICS  
0°C  
25°C  
85°C  
Symbol  
Characteristic  
Input HIGH Current  
Min  
Max  
Min  
Max  
Min  
Max  
Unit  
µA  
µA  
V
Condition  
I
225  
175  
175  
IH  
IL  
I
Input LOW Current  
0.5  
0.5  
0.5  
1
1
1
V
V
V
Input HIGH Voltage  
Input LOW Voltage  
Output Reference Voltage  
3.83  
3.05  
3.62  
4.16  
3.52  
3.73  
3.87  
3.05  
3.65  
4.19  
3.52  
3.75  
3.94  
3.05  
3.69  
4.28  
3.55  
3.81  
VE = 5.0V  
VE = 5.0V  
VE = 5.0V  
IH  
IL  
V
V
BB  
1. PECL V , V , and V  
IH IL  
are referenced to VE and will vary 1:1 with the power supply. The levels shown are for VE = 5.0V.  
BB  
MOTOROLA  
2–2  
MC10H641 MC100H641  
100H PECL DC CHARACTERISTICS  
0°C  
25°C  
85°C  
Symbol  
Characteristic  
Input HIGH Curren  
Min  
Max  
Min  
Max  
Min  
Max  
Unit  
µA  
µA  
V
Condition  
I
I
225  
175  
175  
IH  
Input LOW Current  
0.5  
0.5  
0.5  
IL  
1
1
1
V
V
V
Input HIGH Voltage  
Input LOW Voltage  
Output Reference Voltage  
3.835  
3.190  
3.62  
4.120  
3.525  
3.74  
3.835  
3.190  
3.62  
4.120  
3.525  
3.74  
3.835  
3.190  
3.62  
4.120  
3.525  
3.74  
VE = 5.0V  
VE = 5.0V  
VE = 5.0V  
IH  
V
IL  
V
BB  
1. PECL V , V , and V  
IH IL  
are referenced to VE and will vary 1:1 with the power supply. The levels shown are for VE = 5.0V.  
BB  
AC CHARACTERISTICS (VT = VE = 5.0V ±5%)  
T
J
= 0°C  
T
J
= + 25°C  
T = + 85°C  
J
Symbol  
Characteristic  
Min  
Typ  
Max  
Min  
Typ  
Max  
Min  
Typ  
Max  
Unit  
Condition  
1
t
t
Propagation Delay  
D to Q  
5.00  
5.36  
5.50  
5.86  
6.00  
6.36  
4.86  
5.27  
5.36  
5.77  
5.86  
6.27  
5.08  
5.43  
5.58  
5.93  
6.08  
6.43  
ns  
CL = 50 pF  
PLH  
PHL  
t
Device Skew  
Part–to–Part  
ps  
skew  
2
3
4
1000  
750  
350  
1000  
750  
350  
1000  
750  
350  
CL = 50pF  
CL = 50 pF  
CL = 50 pF  
Single V  
CC  
Output–to–Output  
t
t
Propagation Delay  
LEN to Q  
4.9  
5.0  
6.9  
7.0  
4.9  
4.9  
6.9  
6.9  
5.0  
5.0  
7.0  
7.0  
ns  
ns  
ns  
CL = 50 pF  
CL = 50 pF  
CL = 50 pF  
CL = 50 pF  
PLH  
PHL  
t
t
Propagation Delay  
EN to Q  
PLH  
PHL  
t
r
t
f
Output Rise/Fall  
0.8V to 2.0V  
1.7  
1.6  
1.7  
1.6  
1.7  
1.6  
5
f
t
t
t
Max Input Frequency  
Recovery Time EN  
Setup Time  
65  
65  
65  
MHz  
ns  
MAX  
REC  
S
1.25  
0.75  
0.75  
1.25  
0.75  
0.75  
1.25  
0.75  
0.75  
0.50  
0.50  
0.50  
0.50  
0.50  
0.50  
ns  
Hold Time  
ns  
H
1. Propagation delay measurement guaranteed for junction temperatures. Measurements performed at 50MHz input frequency.  
2. Skew window guaranteed for a single temperature across a V = V = V of 4.75V to 5.25V (See Application Note in this datasheet).  
CC  
3. Skew window guaranteed for a single temperature and single V  
4. Output–to–output skew is specified for identical transitions through the device.  
5. Frequency at which output levels will meet a 0.8V to 2.0V minimum swing.  
T
E
= V = V  
E
CC  
T
DETERMINING SKEW FOR A SPECIFIC APPLICATION  
The H641 has been designed to meet the needs of very low  
skew clock distribution applications. In order to optimize the  
device for this application special considerations are  
necessary in the determining of the part–to–part skew  
specification limits. Older standard logic devices are specified  
with relatively slack limits so that the device can be  
guaranteed over a wide range of potential environmental  
conditions. This range of conditions represented all of the  
potential applications in which the device could be used. The  
result was a specification limit that in the vast majority of cases  
was extremely conservative and thus did not allow for an  
optimum system design. For non–critical skew designs this  
practice is acceptable, however as the clock speeds of  
systems increase overly conservative specification limits can  
kill a design.  
The following will discuss how users can use the  
information provided in this data sheet to tailor a part–to–part  
skew specification limit to their application. The skew  
determination process may appear somewhat tedious and  
time consuming, however if the utmost in performance is  
required this procedure is necessary. For applications which  
do not require this level of skew performance a generic  
part–to–part skew limit of 2.5ns can be used. This limit is good  
fortheentireambienttemperaturerange,theguaranteedV  
CC  
(V ,V )rangeandtheguaranteedoperatingfrequencyrange.  
T
E
2–3  
MOTOROLA  
MC10H641 MC100H641  
Temperature Dependence  
Figure 2 illustrates the thermal resistance (in °C/W) for the  
28–lead PLCC under various air flow conditions. By reading  
the thermal resistance from the graph and multiplying by the  
power dissipation calculated above the junction temperature  
increase above ambient of the device can be calculated.  
A unique characteristic of the H641 data sheet is that the  
AC parameters are specified for a junction temperature rather  
than the usual ambient temperature. Because very few  
designs will actually utilize the entire commercial temperature  
range of a device a tighter propagation delay window can be  
established given the smaller temperature range. Because  
the junction temperature and not the ambient temperature is  
what affects the performance of the device the parameter  
limits are specified for junction temperature. In addition the  
relationship between the ambient and junction temperature  
will vary depending on the frequency, load and board  
environment of the application. Since these factors are all  
under the control of the user it is impossible to provide  
specification limits for every possible application. Therefore a  
baseline specification was established for specific junction  
temperatures and the information that follows will allow these  
to be tailored to specific applications.  
70  
60  
50  
40  
30  
Since the junction temperature of a device is difficult to  
measure directly, the first requirement is to be able to  
“translate” from ambient to junction temperatures. The  
standard method of doing this is to use the power dissipation  
of the device and the thermal resistance of the package. For  
a TTL output device the power dissipation will be a function of  
theloadcapacitanceandthefrequencyoftheoutput. Thetotal  
power dissipation of a device can be described by the  
following equation:  
0
200  
400  
600  
800  
1000  
AIRFLOW (LFPM)  
Figure 2.  
versus Air Flow  
JA  
P
(watts) = I  
(no load) * V +  
CC  
L
D
CC  
* f * C * # Outputs  
V
* V  
S
CC  
Finally taking this value for junction temperature and  
applying it to Figure 3 allows the user to determine the  
propagation delay for the device in question. A more common  
use would be to establish an ambient temperature range for  
the H641’s in the system and utilize the above methodology  
to determine the potential increased skew of the distribution  
where:  
V = Output Voltage Swing = 3V  
S
f = Output Frequency  
C = Load Capacitance  
L
I
= I  
+ I  
network. Note that for this information if the T  
versus  
CC EE CCH  
PD  
Temperature curve were linear the calculations would not be  
required. If the curve were linear over all temperatures a  
simple temperature coefficient could be provided.  
Figure 1 plots the I versus Frequency of the H641 with  
CC  
no load capacitance on the output. Using this graph and the  
information specific to the application a user can determine  
the power dissipation of the H641.  
6.4  
5
4
3
2
1
0
6.2  
6.0  
5.8  
5.6  
5.4  
5.2  
T
PHL  
T
PLH  
110  
–30  
–10  
10  
30  
50  
70  
90  
C)  
130  
0
10  
20  
30  
40  
50  
60  
70  
80  
JUNCTION TEMPERATURE (  
°
FREQUENCY (MHz)  
Figure 3. T  
versus Junction Temperature  
PD  
Figure 1. I  
versus f (No Load)  
CC  
MOTOROLA  
2–4  
MC10H641 MC100H641  
V
Dependence  
CC  
1.15  
1.10  
1.05  
1.00  
0.95  
0.90  
0.85  
0.80  
0.75  
TTL and CMOS devices show a significant propagation  
delay dependence with V . Therefore the V  
variation in a  
CC CC  
system will have a direct impact on the total skew of the clock  
distribution network. When calculating the skew between two  
devices on a single board it is very likely an assumption of  
T
PLH  
identicalV scanbemade.Inthiscasethenumberprovided  
CC  
in the data sheet for part–to–part skew would be overly  
conservative. By using Figure 4 the skew given in the data  
sheet can be reduced to represent a smaller or zero variation  
in V . The delay variation due to the specified V  
is 270ps. Therefore, the 1ns window on the data sheet can  
be reduced by 270ps if the devices in question will always  
experience the same V . The distribution of the propagation  
delay ranges given in the data sheet is actually a composite  
of three distributions whose means are separated by the fixed  
difference in propagation delay at the typical, minimum and  
MEASURED  
variation  
CC  
CC  
T
PHL  
40  
CC  
THEORETICAL  
0
10  
20  
30  
50  
60  
70  
80  
90 100  
maximum V  
.
CC  
CAPACITIVE LOAD (pF)  
Figure 5. T  
versus Load  
PD  
140  
100  
60  
Rise/Fall Skew Determination  
The rise–to–fall skew is defined as simply the difference  
between the T and the T propagation delays. This  
PLH  
PHL  
skew for the H641 is dependent on the V  
device. Notice from Figure 4 the opposite relationship of T  
applied to the  
CC  
PD  
versus V  
between T  
and T  
PLH PHL  
. Because of this the  
CC  
rise–to–fall skew will vary depending on V . Since in all  
CC  
20  
likelihood it will be impossible to establish the exact value for  
V
, the expected variation range for V  
should be used. If  
CC  
CC  
–20  
–60  
–100  
–140  
this variation will be the ±5% shown in the data sheet the  
rise–to–fall skew could be established by simply subtracting  
the fastest T  
1.41ns. If a tighter V  
T
T
PLH  
from the slowest T  
; this exercise yields  
PHL  
PLH  
PHL  
range can be realized Figure 4 can be  
CC  
used to establish the rise–to–fall skew.  
Specification Limit Determination Example  
The situation pictured in Figure 6 will be analyzed as an  
example. Thecentralclockisdistributedtotwodifferentcards;  
on one card a single H641 is used to distribute the clock while  
on the second card two H641’s are required to supply the  
needed clocks. The data sheet as well as the graphical  
information of this section will be used to calculate the skew  
between H641a and H641b as well as the skew between all  
4.75  
4.85  
4.95  
5.05  
VCC (V)  
5.15  
5.25  
Figure 4. T  
versus V  
CC  
PD  
threeofthedevices. OnlytheT  
numbers can be found using the same technique. The  
following assumptions will be used:  
willbeanalyzed,theT  
PLH  
PHL  
Capacitive Load Dependence  
– All outputs will be loaded with 50pF  
– All outputs will toggle at 30MHz  
As with V  
CC  
the propagation delay of a TTL output is  
intimately tied to variation in the load capacitance. The skew  
specifications given in the data sheet, of course, assume  
equal loading on all of the outputs. However situations could  
arise where this is an impossibility and it may be necessary to  
estimate the skew added by asymmetric loading. In addition  
the propagation delay numbers are provided only for 50pF  
loads, thus necessitating a method of determining the  
propagation delay for alternative loads.  
– The V  
variation between the two boards is ±3%  
CC  
– The temperature variation between the three  
devices is ±15°C around an ambient of 45°C.  
– 500LFPM air flow  
The first task is to calculate the junction temperature for the  
devices under these conditions. Using the power equation  
yields:  
Figure 5 shows the relationship between the two  
propagation delays with respect to the capacitive load on the  
output. Utilizingthisgraphandthe50pFlimitsthespecification  
of the H641 can be mapped into a spec for either a different  
value load or asymmetric loads.  
P
= I  
(no load) * V +  
CC  
CC  
D
CC  
V
* V * f * C * # outputs  
S L  
= 1.8 * 48mA * 5V + 5V * 3V * 30MHz *  
50pF * 9  
= 432mW + 203mW = 635mW  
2–5  
MOTOROLA  
MC10H641 MC100H641  
Using the thermal resistance graph of Figure 2 yields a  
thermal resistance of 41°C/W which yields a junction  
temperature of 71°C with a range of 56°C to 86°C. Using the  
the conservative worst case limits provided at the beginning  
of this note. For very high performance designs, this extra  
information and effort can mean the difference between going  
ahead with prototypes or spending valuable engineering time  
searching for alternative approaches.  
T
versus Temperature curve of Figure 3 yields a  
PD  
propagation delay of 5.42ns and a variation of 0.19ns.  
Since the design will not experience the full ±5% V  
variation of the data sheet the 1ns window provided will be  
unnecessarily conservative. Using the curve of Figure 4  
CC  
Card 1  
H641a  
Q0  
shows a delay variation due to a ±3% V  
variation of  
CC  
±0.075ns. Therefore the 1ns window can be reduced to  
1ns – (0.27ns – 0.15ns) = 0.88ns. Since H641a and H641b  
are on the same board we will assume that they will always be  
ECL  
TTL  
Q8  
at the same V ; therefore the propagation delay window will  
CC  
only be 1ns – 0.27ns = 0.73ns.  
Putting all of this information together leads to a skew  
between all devices of  
H641b  
ECL  
Q0  
Q8  
0.19ns + 0.88ns  
(temperature + supply, and inherent device),  
TTL  
while the skew between devices A and B will be only  
0.19ns + 0.73ns  
(temperature + inherent device only).  
Card 2  
In both cases, the propagation delays will be centered  
H641c  
ECL  
around 5.42ns, resulting in the following t  
windows:  
PLH  
Q0  
Q8  
T
T
= 4.92ns – 5.99ns; 1.07ns window  
PLH  
PLH  
TTL  
(all devices)  
= 5.00ns – 5.92ns; 0.92ns window  
(devices a & b)  
Of course the output–to–output skew will be as shown in  
the data sheet since all outputs are equally loaded.  
Figure 6. Example Application  
This process may seem cumbersome, however the delay  
windows, and thus skew, obtained are significantly better than  
MOTOROLA  
2–6  
MC10H641 MC100H641  
OUTLINE DIMENSIONS  
FN SUFFIX  
PLASTIC PLCC PACKAGE  
CASE 776–02  
ISSUE D  
M
S
S
0.007 (0.180)  
T
L–M  
N
B
Y BRK  
D
–N–  
M
S
S
0.007 (0.180)  
T
L–M  
N
U
Z
–M–  
–L–  
W
D
S
S
S
0.010 (0.250)  
T
L–M  
N
X
G1  
V
28  
1
VIEW D–D  
M
S
S
S
A
0.007 (0.180)  
0.007 (0.180)  
T
L–M  
L–M  
N
M
S
S
0.007 (0.180)  
T
L–M  
N
H
Z
M
S
T
N
R
K1  
C
E
0.004 (0.100)  
SEATING  
PLANE  
G
K
–T–  
VIEW S  
J
M
S
S
0.007 (0.180)  
T
L–M  
N
F
G1  
S
S
S
0.010 (0.250)  
T
L–M  
N
VIEW S  
NOTES:  
INCHES  
MILLIMETERS  
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.  
DIM  
A
B
C
E
F
G
H
J
K
R
U
V
W
X
Y
Z
G1  
K1  
MIN  
MAX  
0.495  
0.495  
0.180  
0.110  
0.019  
MIN  
12.32  
12.32  
4.20  
MAX  
12.57  
12.57  
4.57  
0.485  
0.485  
0.165  
0.090  
0.013  
2.29  
2.79  
0.33  
0.48  
0.050 BSC  
1.27 BSC  
4. DIMENSIONING AND TOLERANCING PER  
ANSI Y14.5M, 1982.  
0.026  
0.020  
0.025  
0.450  
0.450  
0.042  
0.042  
0.042  
–––  
0.032  
–––  
–––  
0.456  
0.456  
0.048  
0.048  
0.056  
0.020  
10  
0.66  
0.51  
0.64  
11.43  
11.43  
1.07  
1.07  
1.07  
–––  
0.81  
–––  
–––  
11.58  
11.58  
1.21  
1.21  
1.42  
0.50  
10  
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.  
2
2
0.410  
0.040  
0.430  
–––  
10.42  
1.02  
10.92  
–––  
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).  
2–7  
MOTOROLA  
MC10H641 MC100H641  
Motorola reserves the right to make changes without further notice to any products herein. Motorola makes no warranty, representation or guarantee regarding  
the suitability of its products for any particular purpose, nor does Motorola assume any liability arising out of the application or use of any product or circuit, and  
specificallydisclaims any and all liability, including without limitation consequential or incidental damages. “Typical” parameters which may be provided in Motorola  
datasheetsand/orspecificationscananddovaryindifferentapplicationsandactualperformancemayvaryovertime. Alloperatingparameters,includingTypicals”  
must be validated for each customer application by customer’s technical experts. Motorola does not convey any license under its patent rights nor the rights of  
others. Motorola products are not designed, intended, or authorized for use as components in systems intended for surgical implant into the body, or other  
applicationsintended to support or sustain life, or for any other application in which the failure of the Motorola product could create a situation where personal injury  
ordeathmayoccur. ShouldBuyerpurchaseoruseMotorolaproductsforanysuchunintendedorunauthorizedapplication,BuyershallindemnifyandholdMotorola  
and its officers, employees, subsidiaries, affiliates, and distributors harmless against all claims, costs, damages, and expenses, and reasonable attorney fees  
arising out of, directly or indirectly, any claim of personal injury or death associated with such unintended or unauthorized use, even if such claim alleges that  
Motorola was negligent regarding the design or manufacture of the part. Motorola and  
Opportunity/Affirmative Action Employer.  
are registered trademarks of Motorola, Inc. Motorola, Inc. is an Equal  
How to reach us:  
USA/EUROPE/Locations Not Listed: Motorola Literature Distribution;  
JAPAN: Nippon Motorola Ltd.; Tatsumi–SPD–JLDC, 6F Seibu–Butsuryu–Center,  
P.O. Box 20912; Phoenix, Arizona 85036. 1–800–441–2447 or 602–303–5454  
3–14–2 Tatsumi Koto–Ku, Tokyo 135, Japan. 03–81–3521–8315  
MFAX: RMFAX0@email.sps.mot.com – TOUCHTONE 602–244–6609  
INTERNET: http://Design–NET.com  
ASIA/PACIFIC: Motorola Semiconductors H.K. Ltd.; 8B Tai Ping Industrial Park,  
51 Ting Kok Road, Tai Po, N.T., Hong Kong. 852–26629298  
MC10H641/D  

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