錚?/div>
2
where:
1
脳
(
VOUTN
(
n
)
+
VOUTP
(
n
)
)
is the average value of the output,
2
1023
(VMID 鈥?VFS)
AGND
0
INPUT CODE
VMID
is the average value of the ideal.
MAXIMUM FULL-SCALE OUTPUT VOLTAGE
Figure 5. Transfer Function
The region over which the output voltage varies with input code
is selected by the INV input. When INV is LOW, the output
voltage increases from (VMID 鈥?VFS), (where VFS = the full-
scale output voltage), to VMID as the input code increases from
0 to 1023. When INV is HIGH, the output voltage decreases
from (VMID + VFS) to VMID with increasing input code.
For each value of input code there are then two possible values
of output voltage. When INV is LOW, the output is defined as
VOUTP(n) where n is the input code and P indicates the oper-
ating region where the slope of the transfer function is positive.
When INV is HIGH, the output is defined as VOUTN(n) where n
indicates the operating region where the slope of the transfer
function is negative.
The following conditions limit the range of usable output voltages:
鈥?The internal DACs limit the minimum allowed voltage at the
VMID input to 5.3 V.
鈥?The scale factor control loop limits the maximum full-scale
output voltage to 5.75 V.
鈥?The output amplifiers settle cleanly at voltages within 1.3 V
from the supply rails.
鈥?The common-mode range of the output amplifiers limit the
maximum value of VMID to AVCC 鈥?3.
At any given valid value of VMID, the voltage required to reach
any one of the above limits defines the maximum usable full-
scale output voltage VFSMAX.
VFSMAX is the envelope in Figure 6. The valid range of VMID
is the shaded area.
VFS (V)
AVCC/2
AVCC/2鈥?.3
5.75
4.3
VALID VMID
2
5.3
0
7
AVCC鈥?
AVCC/2
VMID (V)
AVCC鈥?
AVCC
Figure 6. VFSMAX vs. VMID
REV. 0
鈥?1鈥?/div>
                        
                        
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