Power up detection circuit

Miscellaneous active electrical nonlinear devices – circuits – and – Signal converting – shaping – or generating – Synchronizing

Reexamination Certificate

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Details

C327S198000, C327S076000, C327S097000

Reexamination Certificate

active

06204701

ABSTRACT:

TECHNICAL FIELD OF THE INVENTION
This present invention relates to detector circuits and more particularly to power-up/power-down detector circuits.
BACKGROUND OF THE INVENTION
A problem in many integrated circuits is the detection of the initial power-on state. There are many functions which may be needed to perform at initial power-on such as self-testing, clearing garbage data from memory and restoring all elements to a known state and loading saved data.
This is particularly useful for battery-backed or battery operated integrated circuits, which may be used to perform power-management or nonvolatizing functions for an electronic system. If such a component has lost its battery power, it may loose its valid data, and may begin to issue erroneous commands to the system. Thus, a great many types of integrated circuits include a “power-on-reset” circuit to detect when power is applied after a power-down condition, and to issue a reset pulse, which is used to initiate performance of the above named functions.
Two objectives in selecting a power-on reset circuit is that the circuit must not generate the reset pulse when not needed, second, the circuit must generate the reset pulse when it is needed.
Particularly in the design of today's dynamic DRAM memories, latches may be employed to set the state of signals to predetermined logic levels during an active or a precharge portion of a memory cycle. The use of these latches may require a master reset signal to force the state of these signals or logic levels to known value subsequent to the DRAM memory powering up. This operation insures that the DRAM memory is properly conditioned in a low power standby state of the RAM memory while waiting for the first memory cycle to be applied to the RAM memory. An ideal operation, the master reset signal should follow the supply voltage until the supply voltage has reached a sufficient voltage level such that all the signals or logic levels can be reset, and then master reset signal should be returned to ground potential. With the emphasis today on utilizing only very low standby power from battery power backup systems, it is desirable that the circuit that produces this master reset signal consume little or no current once the device has been powered up. Furthermore, this reset signal should be generated every time the RAM memory is powered up regardless of the length of time between subsequent power-up intervals. This generation of the master reset signal regardless of the length of the interval of time insures that despite the power-up sequence of the RAM memory, the state of the RAM memory is properly set for correct and accurate memory operation.
These two requirements, namely that the standby current drain from the circuit to produce the master reset signal has been unsatisfactorily large or the circuit to produce the master reset signal requires an unacceptably long period of time to accurately reproduce the master reset signal between power-ups and downs has not been met by the prior art in one circuit.
FIG. 1
illustrates a power-up detector that provides a power-up detector signal, PUD. This circuit has the disadvantage of producing a large standby current drain from the power supply. The circuit has the following behavior as power is applied to the circuit. Initially nodes
200
,
202
,
204
,
206
and
208
are at V
ss
or ground potential. As V
dd
rises to V
tp
potential, the threshold voltage of p-channel transistor
100
, transistor
100
will turn on. This causes node
200
to charge toward V
dd
potential, forcing node
202
low due to the operation of invertor
110
, node
204
high due to the action of invertor
112
, node
206
low due to the action of invertor
114
and node
208
, PUD, high due to the action of invertor
116
, providing a signal to indicate the power-up condition.
As node
200
charges toward V
dd
, n-channel transistor
106
will turn on, creating a voltage divider between transistor
100
and transistor
106
. Since node
206
has been set low, n-channel transistor
104
is off and transistors
108
and
104
do not conduct current at this time. Transistors
100
and
106
are designed such that the potential on node
200
will not drop below the switching threshold of inverter
110
until V
dd
has reached sufficient potential to assure the proper operation of all internal circuitry and the proper initialization of all internal nodes. As V
dd
reaches the required potential where proper initialization has been achieved, the rate of increase in the potential of node
200
is less than the rate of increase in the switching threshold of inverter
110
.
Thus, the potential on node
200
drops below the switching threshold of invertor
110
. Node
202
is forced high due to the operation of invertor
110
, node
204
is forced low due to the operation of invertor
112
, node
206
is forced high due to the operation of invertor
114
and node
208
, PUD is forced low due the action of invertor
116
, indicating that the power up period has ended. As node
206
goes high it turns on transistor
104
. A discharging path through devices
108
and
104
is thus created that pulls node
200
close to ground, V
ss
, potential. This feedback path is provided to insure that node
200
does not oscillate around the switching threshold of invertor
110
, due to supply noise, and cause multiple PUD signals. Because of the feedback path, there is a continuous current path from V
dd
to V
ss
while the circuit is powered on.
For example, the current may be in the 50 micro amp-range. This is a very significant contribution to the overall current of the device used with the power-up detector and as a consequence resulting in inefficiencies.
FIG. 2
illustrates a power-up detector circuit that effectively eliminates this standby current; however, it has the disadvantage that during a power-up-down-up sequence of short duration, the power-up detector circuit fails to provide a power-up detection signal on the last power-up.
The operation of
FIG. 2
is as follows. Before initial power-up, node
400
is at ground, V
ss
, potential. As V
dd
rises to V
tp
, the threshold voltage of the p-channel transistor in invertor
308
, node
402
, PUD, goes high, providing a signal to indicate the power-up condition. P-channel transistor
306
is designed to have a higher threshold voltage than V
tp
so that it will not turn on before invertor
308
forces PUD high, thereby assuring that transistor
306
remains off. Node
400
will remain low until V
dd
exceeds the sum of the threshold voltage of p-channel transistor
300
and the threshold voltage of p-channel transistor
302
. PUD will remain high until node
400
reaches the switching threshold of invertor
308
. V
dd
must exceed this threshold by the sum of the thresholds of transistors
300
and
302
. This voltage level is sufficient to insure the proper operation of all internal circuitry and to insure the proper initialization of all internal nodes. Once node
400
exceeds the switching threshold of invertor
308
, node
402
is forced low, indicating that the power-up period has ended. When node
402
goes low, transistor
306
is turned on, pulling node
400
to V
dd
potential. This assures that there is no current path in invertor
308
due to an intermediate voltage level on node
400
. This circuit draws no current while the device is powered on.
The circuit of
FIG. 2
has the disadvantage of not detecting a second power-up sequence if it occurs too soon after a power-down. The problem can be seen from the following discussion. Recall that after power-up, node
400
was brought to V
dd
potential. When the device is powered down the only discharge path for node
400
is through transistor
306
. Node
400
will follow the V
dd
supply as it is discharged until V
dd
reaches a potential of V
tp
, where V
tp
is the threshold voltage of p-channel transistor
306
. Thus, when the V
dd
supply is fully discharged to ground, node
400
is still at V
tp
potential. The only way that node
400
can be fully discha

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