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5962-9561101MZC 参数 Datasheet PDF下载

5962-9561101MZC图片预览
型号: 5962-9561101MZC
PDF下载: 下载PDF文件 查看货源
内容描述: [Field Programmable Gate Array, 190MHz, 320-Cell, CMOS, CQFP164, TOP BRAZED, CERAMIC, QFP-164]
分类和应用: 可编程逻辑
文件页数/大小: 76 页 / 730 K
品牌: XILINX [ XILINX, INC ]
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R
XC3000 Series Field Programmable Gate Arrays  
series resistor R2 may be included to add to the amplifier  
output impedance when needed for phase-shift control,  
crystal resistance matching, or to limit the amplifier input  
swing to control clipping at large amplitudes. Excess feed-  
back voltage may be corrected by the ratio of C2/C1. The  
amplifier is designed to be used from 1 MHz to about  
one-half the specified CLB toggle frequency. Use at fre-  
quencies below 1 MHz may require individual characteriza-  
tion with respect to a series resistance. Crystal oscillators  
above 20 MHz generally require a crystal which operates in  
a third overtone mode, where the fundamental frequency  
must be suppressed by an inductor across C2, turning this  
parallel resonant circuit to double the fundamental crystal  
frequency, i.e., 2/3 of the desired third harmonic frequency  
network. When the oscillator inverter is not used, these  
IOBs and their package pins are available for general user  
I/O.  
Crystal Oscillator  
Figure 18 also shows the location of an internal high speed  
inverting amplifier that may be used to implement an  
on-chip crystal oscillator. It is associated with the auxiliary  
buffer in the lower right corner of the die. When the oscilla-  
tor is configured and connected as a signal source, two  
special user IOBs are also configured to connect the oscil-  
lator amplifier with external crystal oscillator components  
as shown in Figure 19. A divide by two option is available to  
assure symmetry. The oscillator circuit becomes active  
early in the configuration process to allow the oscillator to  
stabilize. Actual internal connection is delayed until com-  
pletion of configuration. In Figure 19 the feedback resistor  
R1, between the output and input, biases the amplifier at  
threshold. The inversion of the amplifier, together with the  
R-C networks and an AT-cut series resonant crystal, pro-  
duce the 360-degree phase shift of the Pierce oscillator. A  
D
Q
Internal  
External  
Alternate  
Clock Buffer  
XTAL1  
XTAL2  
(IN)  
R1  
R2  
Suggested Component Values  
R1 0.5 – 1 MΩ  
R2 0 – 1 kΩ  
Y1  
(may be required for low frequency, phase  
shift and/or compensation level for crystal Q)  
C1, C2 10 – 40 pF  
Y1 1 – 20 MHz AT-cut parallel resonant  
C1  
C2  
100 PIN  
CQFP PQFP  
164 PIN 175 PIN 176 PIN 208 PIN  
44 PIN 68 PIN  
84 PIN  
132 PIN 160 PIN  
CQFP  
105  
PGA  
T14  
P15  
TQFP  
91  
PQFP  
110  
PLCC  
30  
PLCC PLCC PGA  
PGA  
P13  
M13  
PQFP  
82  
XTAL 1 (OUT)  
XTAL 2 (IN)  
67  
61  
82  
76  
47  
43  
57  
53  
J11  
L11  
26  
99  
85  
100  
76  
X7064  
Figure 19: Crystal Oscillator Inverter. When activated, and by selecting an output network for its buffer, the crystal  
oscillator inverter uses two unconfigured package pins and external components to implement an oscillator. An optional  
divide-by-two mode is available to assure symmetry.  
7-18  
November 9, 1998 (Version 3.1)  
 
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