NCP2809 Series
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13
TYPICAL CHARACTERISTICS
Figure 38. Turning–On Time/V
p
= 5.0 V
and F = 100 Hz
Ch1 = OUT_R, Ch2 = VMC and Ch3 = Shutdown
Figure 39. Turning–On Time Zoom/V
p
= 5.0 V
and F = 400 Hz
Ch1 = OUT_R, Ch2 = VMC and Ch3 = Shutdown
Figure 40. Turning–Off Time/V
p
= 5.0 V
and F = 100 Hz
Ch1 = OUT_R, Ch2 = VMC and Ch3 = Shutdown
Figure 41. TurningOff Time Zoom/Vp = 5.0 V
and F = 400 Hz
Ch1 = OUT_R, Ch2 = VMC and Ch3 = Shutdown
NCP2809 Series
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APPLICATION INFORMATION
Detailed Description
The NCP2809 power audio amplifier can operate from
2.6 V to 5.0 V power supply. It delivers 24 mW
rms
output
power to a 16 load (V
P
= 2.4 V) and 131 mW
rms
output
power to a 16 load (V
P
= 5.0 V).
The structure of NCP2809 is basically composed of two
identical internal power amplifiers; NCP2809A has a fixed
internal gain of 0 dB and the gain can be set externally with
the NCP2809B.
Internal Power Amplifier
The output P
mos
and N
mos
transistors of the amplifier are
designed to deliver the specified output power without
clipping. The channel resistance (R
on
) of the N
mos
and P
mos
transistors does not exceed 3.0 when driving current.
The structure of the internal power amplifier is
composed of three symmetrical gain stages, first and
medium gain stages are transconductance gain stages in
order to maximize bandwidth and DC gain.
TurnOn and TurnOff Transitions
A Turnon/off transition is shown in the following plot
corresponding to curves in Figures 38 to 41.
In order to eliminate “pop and click” noises during
transitions, output power in the load must be slowly
established or cut. When logic high is applied to the
shutdown pin, the bypass voltage begins to rise
exponentially and once the output DC level is around the
common mode voltage, the gain is established slowly
(50 ms). This way to turnon the device is optimized in
terms of rejection of “pop and click” noises.
A theoretical value of turnon time at 25°C is given by
the following formula.
C
by
: Bypass Capacitor
R: Internal 300 k resistor with a 25% accuracy
T
on
= 0.95 * R * C
by
When logic is turned low on shutdown pin, the device
enters in shutdown mode:
50 ms later the audio signal is cut off as the gain is
turned to zero internally as shown in Figure 41.
385 ms later, the DC signal will reach 0.7 V due to
exponential discharge of the bypass voltage. It is then tied
to Ground as shown in Figure 40.
A theoretical approach of this time is:
T
off
= R * C
by
* Ln(V
p
/1.4)
Shutdown Function
The device enters shutdown mode when shutdown signal
is low. During the shutdown mode, the DC quiescent
current of the circuit does not exceed 600 nA.
Current Limit Protection Circuitry
The maximum output power of the circuit (P
Orms
=
135 mW, V
P
= 5.0 V, R
L
= 16 ) requires a peak current in
the load of 130 mA.
In order to limit excessive power dissipation in the load
when a shortcircuit occurs, the current limit in the load is
fixed to 250 mA. The current in the output MOS transistors
is realtime monitored, and when exceeding 250 mA, the
gate voltage of the corresponding MOS transistor is clipped
and no more current can be delivered.
Thermal Overload Protection Circuitry
Internal amplifiers are switched off when temperature
exceeds 160°C, and will be switched back on only when the
temperature goes below 140°C.
NCP2809 is a stereo power audio amplifier.
If the application requires a Single Ended topology with
output coupling capacitors, then the current provided by
the battery for one output is as following:
V
O
(t) is the AC voltage seen by the load. Here we
consider a sine wave signal with a period T and a peak
voltage V
O
.
R
L
is the load.
T
TIME
T/2
V
O
/R
L
I
p
(t)
So, the total power delivered by the battery to the device is:
P
TOT
+ V
p
I
p
avg
I
p
avg +
1
2
ŕ
0
V
o
R
L
sin(t)dt +
V
o
.R
L
P
TOT
+
V
p
.V
o
.R
L
The power in the load is P
OUT
.
P
OUT
+
V
O
2
2R
L
NCP2809 Series
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15
The dissipated power by the device is
P
D
+ P
TOT
* P
OUT
P
D
+
V
o
R
L
ƪ
V
P
*
V
O
2
ƫ
At a given power supply voltage, the maximum power
dissipated is:
P
Dmax
+
V
P
2
2
2
.R
L
Of course, if the device is used in a typical stereo
application, each load with the same output power will give
the same dissipated power. Thus the total lost power for the
device is:
P
D
+
V
o
R
L
ƪ
2V
P
* V
O
ƫ
And in this case, the maximum power dissipated will be:
P
Dmax
+
V
P
2
2
.R
L
In single ended operation, the efficiency is:
+
.V
O
2V
P
If the application requires a NOCAP scheme without
output coupling capacitors, then the current provided by
the battery for one output is as following:
V
o
(t) is the AC voltage seen by the load. Here we
consider a sine wave signal with a period T and a peak
voltage V
O
.
R
L
is the load.
T
TIME
T/2
V
O
/R
L
I
p
(t)
So, the total power delivered by the battery to the device is:
P
TOT
+ V
p
I
p
avg
I
p
avg +
1
ŕ
0
V
o
R
L
sin(t)dt +
2V
o
.R
L
P
TOT
+
2V
p
.V
o
.R
L
The power in the load is P
OUT
P
OUT
+
V
O
2
2R
L
The dissipated power by the device is
P
D
+ P
TOT
* P
OUT
P
D
+
V
o
R
L
ƪ
2V
P
*
V
O
2
ƫ
At a given power supply voltage, the maximum power
dissipated happens when V
O
= Vp/2.
P
Dmax
+
0.19V
P
2
R
L
Of course, if the device is used in a typical stereo
application, each load with the same output power will give
the same dissipated power. Thus the total lost power for the
device is:
P
D
+
V
o
R
L
ƪ
4V
P
* V
O
ƫ
And in this case, the maximum power dissipated will be:
P
Dmax
+
0.38V
P
2
R
L
In NOCAP operation, the efficiency is:
+
.V
O
4V
P
GainSetting Selection
With NCP2809 Audio Amplifier family, you can select
a closedloop gain of 0db for the NCP2809A and an
external gain setting with the NCP2809B. In order to
optimize device and system performance, NCP2809 needs
to be used in low gain configurations. It minimizes THD+N
values and maximizes the signaltonoise ratio, and the
amplifier can still be used without running into the
bandwidth limitations.
NCP2809A can be used when a 0 dB gain is required.
Adjustable gain is available on NCP2809B.
NCP2809 Amplifier External Components
Input Capacitor Selection (C
in
)
The input coupling capacitor blocks the DC voltage at
the amplifier input terminal. This capacitor creates a
highpass filter with the internal (A version with 20 k) or
external (B version) resistor. Its cutoff frequency is given
by:
f
c
+
1
2* *R
in
*C
in
(eq. 1)
The size of the capacitor must be large enough to couple
in low frequencies without severe attenuation. However a
large input coupling capacitor requires more time to reach
its quiescent DC voltage (V
P
/2) and can increase the
turnon pops.
An input capacitor value of 100 nF performs well in
many applications (in case of R
in
= 20 k).

NCP2809ADMR2G

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Audio Amplifiers 135mW Stereo Audio PWR Industrial Temp
Lifecycle:
New from this manufacturer.
Delivery:
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