ivtech
New User
Jul 11, 2008, 1:53 AM
Post #16 of 32
(5007 views)
Shortcut
|
|
Re: [ivtech] RCA 25 inch picturetube type.
[In reply to]
|
Can't Post
|
|
You should measure volts with DC not AC and you don't need to turn on the tv, just plug in the cord,and measure the way i suggested.and about The CTC203 you should have like ctc203ad5/AX and so on give those letters and #,s after ctc203??????
Also look at L14401 take this coil out scrap its leggs and resolder back,also you may have to replace the hot,also check this info below. Power Supply 11
Figure 2-1, CTC203 Main Power Supply Block Diagram
POWER
OUTPUT
Q14101
BIAS
SUPPLIES
OUTPUT
POWER
TRANSFORMER
T14101
OPTO-ISOLATOR
U14101
+16Vr
+5.2Vs
-12Vr
+33Vs
+7.6Vr
Reg B+
Feedback
Reg B+
CONTROL
LATCH
Q14102/103
PRECISION
REGULATOR
U14102
OVER-CURRENT
OVER-VOLTAGE
R14108
Raw B+
Cold Ground
Hot Ground
The main supply generates voltages for normal operation of all other circuits and
components. In addition, many of the supplies are used to generate the remainder of
the low and high voltages required by the chassis.
The Technical Training Manual will discuss the power supplies in this order; Main,
Switched (SW) and Scan Derived.
12 Power Supply
Figure 2-2, Power Supply Output Device Waveforms
Q14101
Drain Voltage
Q14101
Gate Voltage
Q14101
Drain Current
Standby Supply Overview
The standby supply is a new class of high power, ZVS (Zero Voltage Switching)
supply developed to minimize switching losses and radiated noise. A return to
discrete devices lowered parts count and decreased circuit board space utilization.
ZVS refers to the ability of the supply causing the voltage across the principal power
output device, to reduce to near zero before the device is switched on. Yet it has a
slow enough time lag to allow the device to switch off completely before any
appreciable voltage is present across the device. This can better be illustrated in
Figure 2-2.
Note that the first two waveforms are voltages, while the third is current. The
MOSFET begins conducting current when the gate voltage reaches the proper turn
on point. From that time, output current rises linearly due to the inductance of the
output transformer. However, notice that once the gate voltage goes high, the drain
voltage decreases almost to zero volts. This eliminates much of the heat dissipation
normally required of an output device.
By reducing the switching losses to almost
zero, the efficiency of the power supply is
greatly increased and the limiting of the
switching voltages causes a substantial
reduction of switching noise.
Also note that by utilizing the resonant
recapture of energy stored in the leakage
inductance of the output transformer, neither
a snubber nor a clamp is required, leading to
improved efficiency and lower parts count.
Power Supply 13
Digital Latches
Before wading deeper into the CTC203 power supply, the technician should become
familiar with the control circuitry used to turn the power output devices on and off. It will
be common to various ZVS supplies used throughout this and other TCE chassis'.
The control switches act similar to an SCR, but with a few variations. Figure 2-3 shows a
truth table and simplified schematic representaion of the power supply control latch shown
in Figure 2-4. Again, while the other ZVS supplies may have slight variations, the basic
concept and operation is the same.
Q1 and Q2 form the basic latch circuit. Both are switching transistors that saturate when
tripped on. In this case an NPN and PNP are used to force the desired results on the output.
The latch is controlled by placing or removing voltages on either base while sufficient
voltage is present on Q2-E to set the latch. Keep in mind B+ will supply drive to the output
when the latches are off!!! The latch REMOVES the output. Any time the truth table
shows a low (0) condition, output is removed.
In condition A, both IN1 and IN2 are low (0). A low in Q2-B turns it on providing a current
path from B+ through R5, R2, Q2-E/C and R3 to ground. Sufficient bias is developed
across R3 to turn Q1 on, setting the latch. Now, regardless of what happens on IN1, the
latch is set. The combined voltage drop on R3 and Q2-E/C places Q2-E at a very low
voltage, shutting the output off.
If IN2 goes high (1) as in condition B, there will be no effect on the output. The high on
IN2 would turn Q1 on, but since it is already on the result is no change in the output state.
In condition D, both inputs are high. A high on Q1-B turns it on. When it turns on it
saturates, bringing Q2-B low, turning it on. When it turns on the latch is again set and the
output goes low.
Condition C is the most difficult to understand because it relies on the input voltages being
different before the latch is tripped. If IN1 is high, the latch state is dependant upon IN2 for
its output state. If IN2 is low, the output is high. If IN2 is high, the output is low.
However, if the latch is set
(tripped) Q2 saturates and holds
Q1 on even with IN1 high. What
has to happen before the latch
will trip off is the loss of bias on
Q1-B.
As IN2 decreases it begins to
divert current flow away from
R3 and its voltage drop also
begins to decrease. The voltage
on Q1-B will eventually drop low
enough for it to shut off. If IN1
is still high Q2-B is now high
and it also shuts off. This
removes both Q1 and Q2 from
the circuit and B+ now supplies
the output voltage.
Figure 2-3, Digital Latch & Truth Table
R3
3300
Q2
R4
1000
R2
1000
B+
R1
1000
Q1
IN 1
IN 2
Out
IN1 IN2 OUT
0 0 0
1 0 1
0 1 0
1 1 0
A
B
C
D
R5
680K
14 Power Supply
Control Latch Review
Now that the digital latch operation is
understood, it needs to be shown how it is used
to regulate the CTC203 power supply. Using
the simplified digital latch schematic from the
previous page, when IN1 is high, IN2 may be
used to control the output. When IN2 is high,
the output is low. When IN2 is low, the output
is high. In Figure 2-4A, Q1-E is grounded.
Normal PN junction drop of a transistor dictates
that a bias of at least +0.6V must be placed on
Q1-B to turn it on.
In Figure 2-4C Q1-E is connected to a
negative 5V supply. The current to turn
the PN junction of Q1 on remains the same.
Now the voltage on Q1-B need only be
0.6V higher than Q1-E, or about -4.4V.
In this manner, the voltage that triggers Q1
may be varied and used to control the output
of the latch. By understandby this circuit,
the regulation and protection of the power
supply may be more fully understood.
Figure 2-4A, Digital Latch Normal
R3
3300
Q2
R2
1000
B+
R1
1000
Q1
IN 1
IN 2
Out
R5
680K
+0.6V
R3
3300
Q2
R2
1000
B+
R1
1000
Q1
IN 1
IN 2
Out
R5
680K
+1.0V
R5
1000
Figure 2-4B
R3
3300
Q2
R2
1000
B+
R1
1000
Q1
IN 1
IN 2
Out
R5
680K
-4.4V
-5V
Supply
Figure 2-4C
In Figure 2-4B a resistor (R5) has been placed
in the emitter circuit of Q1. The resistance of
R5 reduces the amount of current through the
PN junction of Q1E/B with the same voltage
on Q1-B. Thus, to increase current high
enough to turn on Q1, Q1-B voltage must
increase. In this case to about +1.0V.
Power Supply 15
Figure 2-5, Power Supply Control Latch
Latch Circuit
Figure 2-5 is the control latch for the CTC203 power supply. It is not much different
from the simplified schematic in Figure 2-3, however there are some additional
circuits that will need to be discussed later.
When power is first applied to the chassis, Raw B+ is available on the "IN1" line at
the junction of Q14103-C and Q14102-B. Since there is no bias difference from
Q14102B-E, it is off and the latch is off. Raw B+ now supplies gate drive to the
output device Q14101-G, turning it on providing output transformer current. At this
time, "IN1" is high, IN2 is low and the latch is off, allowing gate drive.
As current builds in the output device, a voltage is developed accross R14108.
When this voltage increases enough, it will bias Q14103 on, which also turns on
Q14102, setting the latch. A current path now exists between Raw B+, R14103,
R14106, Q14102-C/E, R14110 and a negative bias voltage developed from the
output transformer.
Once the latch is set, Q14102-E voltage and output drive is removed and the output
device, Q14101 shuts off. With output current dropping, the corresponding voltage
drop across R14108 begins to decrease along with the negative bias supply. At some
point the voltage at Q14103-B drops low enough to allow it to turn off. When it
does, bias is removed from Q14102-B and it shuts off. When it shuts off, gate drive
is again allowed to turn the output device, Q14101 on and output current begins to
build once more.
As the power supply circuits develop, it will be seen that by either varying the bias
voltage on Q14103-B while maintaining the voltage on Q14103-E, or varying the
bias on Q14103-E, while maintaining the voltage on Q14103-B, the on/off time of
the latch can be controlled precisely. Controlling the latch means output current is
also controlled. The off time of the latch is reasonbly constant. It is the "on" time of
the output that controls the supply voltages.
CR14105
R14108
0.1
3W
Q14102
R14109
750
R14107
43
Q14101
To Output
Transformer
T14101
R14103
1Meg
R14104
3300
R14106
1000
R14110
22K
Q14103
Raw B+
Positive Bias
Supply
IN1
IN2
OUT
16 Power Supply
Main Supply Block Diagram
The Main Supply distributes power to all devices that need to remain "alive" when
the chassis is "off". In addition, it must retain enough power to keep the
microprocessor active during a power failure event long enough to exercise the
"batten down the hatches" routine leading to a graceful shutdown of the chassis
before power disappears completely. ("Batten" is a software routine which stores
off all customer settings and chassis alignments to the EEPROM. This enables the
set to start normally after a catastrophic power failure.)
The voltages available during standby operation are:
• -12 volts
• +5.2 volts
• +7.6 volts
• +16 volts
• +33 volts
• Reg B+
The supply converts raw B+ from the incoming AC line into the various DC supplies
required by the CTC203. There is a "Data Acquisition" mode requiring greater
current supply demands from the supply than normally needed during standby, but
less than is needed during full run operation. For instance, during a TVGuide+
download, there is no reason for the set to display a picture, however, the tuner must
be active to receive the signal. This requires more current from Reg B+ from which
the +33V supply is derived.
Since the forward conduction mode is used, the driver current is proportional to the
supply current and higher frequencies (70-90 kHz) may be used for greater efficiency.
The standby supply may be broken into several sections according to Figure 2-5.
The Latch circuit (discussed previously) consists of Q14102 and Q14103. They
control the off/on time of the output device, Q14101.
Current in the output power transformer, T14101, transferred to the secondary, is
used to generate the various supplies from Raw B+ provided by the main rectifier
from incoming AC.
The regulator, U14102 and opto-isolator, U14101 provide regulation of the +16Vs
supply and isolation between the cold ground run supplies and the hot ground
generator circuit components.
Overcurrent and overvoltage protection of the output device is provided by resistor
R14108 in series with Q14101.
Power Supply 17
Figure 2-6, CTC203 Main Supply Block Diagram (Standby Voltages)
POWER
OUTPUT
Q14101
BIAS
SUPPLIES
OUTPUT
POWER
TRANSFORMER
T14101
OPTO-ISOLATOR
U14101
+16Vr
+5.2Vs
-12Vr
+33Vs
+7.6Vr
Reg B+
Feedback
Reg B+
CONTROL
LATCH
Q14102/103
PRECISION
REGULATOR
U14102
OVER-CURRENT
OVER-VOLTAGE
R14108
Raw B+
Cold Ground
Hot Ground
AC Input and Degaussing
Raw AC is connected using protection (F14200) and filtering/smoothing components
to assure spikes and unexpected surges do not cause catastrophic failure.
Degaussing may only be done when the +12V run supply is active. System Control
sends a high out during startup turning on Q14201. As long as the +12Vr supply is
up, relay K14201 is turned on activating the contacts on pins 3 & 4. Current from the
AC line is now routed to the degaussing coil. Degaussing occurs as long as thermal
resistor RT14250 allows. It provides an exponential decay of current to the degaussing
coil. Degauss current must be allowed to decay before the relay stops all degauss
coil current to allow proper degaussing, otherwise color non-uniformity will result.
When System Control removes the active deguass signal, Q14201 shuts off, removing
drive current from the relay coil, breaking the contacts and removing AC power
from the degaussing coil. The degaussing cycle is then complete.
RT14201
K14201
3
4
2
1
+12VrSW
Q14201
CR14250
J14203
DEGAUSSING
COIL
From Incoming
AC Line
U13101
SYSTEM
CONTROL
45
R14206
1000
Degauss: High
Figure 2-7, Degaussing
18 Power Supply
Figure 2-8, AC Input
Raw B+
Incoming AC (95 - 135 VAC) is input through an LCI (Line Conducted Interference)
filter consisting mainly of T14201 and several filter capacitors. Raw B+ is generated
from the incoming AC by a discrete bridge rectifier circuit consisting of CR14201,
CR14202, CR14203 and CR14204. Main power supply input voltage is 95-135
VAC to provide a Raw B+ voltage of about +156V depending upon the chassis
version. Generally, larger screen sizes will require higher raw B+.
156VDC
120VAC Raw B+
F14201
5A
TP14210
C14205
680uF C14206
0.012
To DeGauss
Circuit
CR14202 CR14201
CR14204 CR14203
T14201
Power Supply 19
Figure 2-9, Main Power Supply
Main Supply Operation
To simplify the understanding of the standby supply (shown in Figure 2-9), it will be
broken down into smaller blocks. These blocks operate somewhat independently,
but ultimately must all function together for proper operation of the supply.
The sections are:
Output
Drive
Control
Feedback/Regulation
Bias Supplies
T14101
9
5
16
14
15
13
10
11
12
Q14102
Q14101
Q14103
3
8
R14107
43
R14106
2000
C14101
2.2uF CR14110
CR14106
CR14108
C14122
33uF
C14122
33uF
CR14107
33V
C14121
3.3uF
C14114
3.3uF
L14102
R14124
3.3
2W
Reg B+
R14109
750
R14110
22K
C14108
0.047
C14104
0.047
CR14103
CR14104
R14108
0.1
3W
R11513
4700
CR11504
18V
Q11501
R14103
1Meg
R14104
3300
R14101
47K
R14102
6800
CR14101
47V
CR14102
CR14105
C14108
1100
1.6KV
RAW B+
Neg Hot
Bias Supply
Neg Hot
Bias Supply
Pos Hot
Bias Supply
Pos Hot
Bias Supply
R14105
10
R14113
1300
R14112
680
U14101
U14102
+16Vs
CR14117
16V
+33Vs
+16Vs
+7.6Vs
+5.2Vs
-12Vs
-12Vr
CR11505
NC
U14103
+5.2V
Reg
+12VrSW
-12V
Fil
C14116
R141111 47uF
10K
Q14107
Q14106
R14126
37.4K
CR14111
R14115
143K
R14116
2000
R14127
10K
R14128
680K
+13Vr
+16Vs
RegB+Vs
Feedback/Regulation
Output
Control Drive
Bias Supplies
20 Power Supply
Standby Supply Startup
A voltage divider network from Raw B+ consisting of R14103 and R14107 provides
the initial positive gate voltage for output MOSFET Q14101 to begin conduction. As
current begins to flow in the output transformer T14101, winding 3/8, feedback current
is induced to windings 1/2. This winding provides several bias voltages to the supply
drivers and feedback circuit, but initially is used to increase the gate voltage, using
C14101 to couple the transformer to the gate. The voltage at pin 9 is increasing in a
positive direction as current increases in the primary. This rising voltage eventually
causes the output, Q14101, to saturate, beginning the first cycle of operation.
As current through Q14101 increases, the voltage drop across current sense resistor
R14108 increases until a threshold is reached. (This threshold is discussed in the
control latch section.) At the time the threshold is reached, the regenerative switch
(latch circuit) consisting of Q14102/Q14103 turns on, removing gate drive from output
device Q14101.
Current flow through Q14101 drops quickly to zero and energy stored in the transformer
primary winding is transferred to C14108 which charges with the negative potential at
Q14101-D. This rising voltage appears across the secondary winding.
When the secondary side of the transformer conducts, the energy stored in the primary
of T14101 is delivered to the secondary supply capacitors and the load. After the
secondary diodes stop conducting, energy still contained in C14108 drives the drain
voltage of Q14101 toward zero. When the drain voltage attempts to go below zero, an
internal diode clamps it near ground.
Now the voltage of T14101 drive winding, 5/9, goes positive and if the latch circuit
allows it, will turn on Q14101 and the next cycle begins. Once the initial startup pulse
from Raw B+ starts the cycle, this bias supply takes over and continues to supply gate
drive to the output device.
Figure 2-10, Power Device Start up Current Flow
Part of
T14101
Q14102
Q14101
Q14103
3
8
R14107
43
R14106
2000
C14101
2.2uF
R14109
750
R14108
0.1
3W
R14103
1Meg
R14104
3300
R14101
47K
R14102
6800
CR14101
47V
CR14102
CR14105
C14108
1100
1.6KV
RAW B+
From
Regulator
Circuits
Bias Supply
from T14101
Windings 9/5
Power Supply 21
Output
Q14101 provides all transformer primary winding drive current. It is a power mosfet
which conducts current from source to drain when the gate voltage is high. Once on,
gate voltage must be reduced to around zero or the drain-source current path must be
interrupted to stop output current. During conduction, current flows from common
(hot) through R14108, Q14101 and T14101 primary winding to Raw B+. C14108 is
used to "tune" the resonant frequency of the primary for better power transfer.
Normally this frequency is around 90kHz during standby and 40-60kHz during run
operation. Figure 2-11 shows the driver and output voltages and a waveform
comparing Q14101-D outputs in standby and run mode. As current flows through
the primary, flux lines induce current flow into secondary windings 5/9, 11/12,
13/15 and 14/16. Typical AC voltages generated from the windings are shown in
Figure 2-12.
Figure 2-12, Typical Secondary Winding Voltages
Figure 2-11, Main Supply Output
T14101
9
5
16
14
15
13
10
11
12
CR14110
CR14106
CR14108
C14122
33uF
C14122
33uF
CR14107
33V
C14121
3.3uF
C14114
3.3uF
L14102
R14124
3.3
2W
Reg B+
R11513
4700
CR11504
18V
Q11501
+33Vs
+16Vs
+7.6Vs
+5.2Vs
-12Vs
-12Vr
NC
U14103
+5.2V
Reg
+12VrSW
-12V
Fil
C14116
47uF
Bias Supply
Windings
Q14101
3
8
R14107
43
C14101
2.2uF
R14108
0.1
3W
C14108
1100
1.6KV
RAW B+
T14101 Pin # AC Voltage
3/8 400 p-p
5/9 15 p-p
11/12 26 p-p
13/15 35 p-p
14/16 250 p-p
22 Power Supply
Figure 2-13, Main Supply Output Drive Control
Standby Supply Drive
To assist the understanding of the control circuit, this discussion will not take the
positive bias supply in consideration at this time. Operation of the control circuit
will be identical.
At initial startup, R14103 provides the gate voltage to turn Q14101 on, providing
primary current. As Q14101 begins to conduct, primary winding current increases,
increasing voltage across the winding and inducing current flow to all secondary
windings. Q14101 quickly saturates.
R14108 monitors the primary winding current, which is also the current through the
output device, Q14101. As this current increases, the corresponding voltage drop
across R14108 increases. When it reaches a voltage high enough to turn Q14103 on,
the latch "sets" stopping drive to the output, Q14101. It does this do to a current path
from common through CR14105, Q14103-E/B, Q14102, R14106 the gate drive
being developed by C14101 and T14101 windings 5/9. Q14102 emitter drops to a
low voltage, shutting the output device Q14101 off. This cuts current flow to the
primary of T14101. Without drain current, drain voltage now increases due to back
EMF across the transformer windings. The secondary diodes conduct and power is
delivered to the loads. C14108 helps shape the waveform, limiting conduction time
as Q14101 shuts off and drain voltage is driven to zero.
Two things are now happening. First, with Q14101 now off, primary current flow
begins to decrease. Second, with current flow in the primary and output stopped, the
voltage across R14108 now decreases below the bias point of Q14103 and it shuts
off, shutting off Q14102. The bias supply developed from T14101-5/9 and C14101
now supplies gate drive and the output, Q14101 turns back on. The process now
begins again.
CR14105
R14108
0.1
3W
Q14102
R14109
750
R14107
43
Q14101
To Output
Transformer
T14101
R14103
1Meg
R14104
3300
R14106
1000
R14110
22K
Q14103
Raw B+
Positive Bias
Supply
IN1
IN2
OUT
Power Supply 23
Figure 2-14, Bias Supplies
Bias Supplies
There are two supplies generated during standby supply operation used to internally
bias the control and regulation components of the supply. Both cycles of the
transformer waveform are utilized to provide a positive and negative supply voltage.
These voltages vary with respect to the current flow in the primary winding of
T14101 but should normally be within the 5 to 10 volt range, positive and negative
respectively. An unrectified pulse is used as the initial gate pulse to saturate the
output device.
Standby Supply Control
Without some form of regulation, the power supply will quickly reach a nominal
output voltage using the control circuit in Figure 2-13. Figure 2-15 again shows the
control circuitry, but adding regulation to keep the output voltages from the secondary
of the supply within design limits. Load variations are constant and there is the
problem of loads outside the normal expected variations to deal with. The main
supply is required to provide standby and run power to some circuits, further
complicating load demands.
All this means that the supply must be regulated and protected against overload
conditions. An opto-isolator protects the "hot" primary side of the supply from the
"cold" secondary side and is also used for regulation.
Referring back to Figure 2-13, it may be seen that by varying the on/off time of the
latch, Q14102 and Q14103, output current can also be varied. For instance, the trip
voltage required to turn Q14103 on with diode CR14105 in its emitter circuit is
about +1.2V. This assumes a PN junction IR drop of 0.6V for the diode and 0.6V for
the emitter-base junction of the transistor. If a second diode were placed in series
with CR14105, the trip voltage would now be +1.8V. (Of course, with the added IR
drop of R14109, the voltage would need to be greater.) If CR14105 were removed,
the trip voltage now would be lower by 0.6V or about +0.6V.
Now it can be seen that regulating the output current by varying IN2 is a matter of
either increasing the voltage on Q14103-B, or lowering the voltage on Q14103-E.
Either method achieves the same results. This technique may be used to provide
regulation of output current.
Negative Supply
Source
(app -5 to -15V)
Positive Supply
Source
(app +5 to +15V)
To Q14101-G
CR14104
C14066
0.047uF
R14601
100
CR14105
C14103
0.047uF
T14101
C14101
2.2uF
9
5
24 Power Supply
Main Power Supply Regulation
To provide regulation of the control latch which in turn varies the secondary
voltages, a regulation circuit is used. Since the regulator is monitoring secondary
voltages which use "cold" ground, and manipulating circuits on the primary or "hot"
side of the power supply transformer, the regulator must also provide isolation.
Initially, a bias voltage is set up on Q14103-B by a voltage divider network between
the positive and negative bias supplies. R14112, the output of U14101 and R14111
make up this network. Since the supplies are constantly changing do to primary
current, they are difficult to measure, however when operating normally the nominal
voltage on Q14103-B is very close to zero.
A feedback voltage, Reg B+, is used to monitor the secondary voltages generated by
the main supply. If Reg B+ increases such that the junction of R14115 & R14116
rises above +2.5 volts, the internal impedance of U14102 (See the Tech Tip on this
new device) decreases. Increased current through the device turns on
opto-isolator, U14101 harder and the output impedance of this device decreases.
This output is in the voltage divider network between the negative and positive bias
supplies. As the impedance decreases, the voltage on Q14103-E goes more negative.
It now takes less voltage on Q14603-B to trip the control latch to the "ON"
condition. Remember that when the latch is on, gate drive is removed from the
output device, Q14101, and output current stops. Secondary supply voltages begin
to drop.
The waveform shows voltage levels on the emitter of U14101 (Top) and the collector
(Bottom). The emitter is essentially the negative supply ripple. The DC level is
about -11V. The internal impedance of the output section is increasing and decreasing
at such a rate that under normal load levels it fluctates closely around 0V.
Figure 2-15, Standby Supply Regulation
Neg Hot
Bias Supply
Pos Hot
Bias Supply
Q14107
Q14106
R14126
37.4K
CR14111
R14115
143K
R14116
2000
R14127
10K
R14113
1300
R14111
10K
R14112
680
R14128
680K
U14101
+13Vr U14102
+16Vs
+16Vs
Reg B+
CR14117
16V
To Control
Q14103-E
Power Supply 25
When Reg B+ drops sufficiently, the junction of R14115 & R14116 drops below
+2.5V. Now the internal impedance of U14102 increases. As it increases, the output
section of the opto-isolator, U14101 is driven less and its impedance also increases.
The voltage on the collector of U14101 now goes towards the positive supply. This
voltage is also on Q14103-E. It now takes more voltage on Q14103-B to turn the
control latch off. Gate drive is allowed on the output, Q14101 and primary winding
current is again available in T14101. As current in the primary increases, voltage in the
secondaries also increases and the cycle repeats.
If a failure occurs in the regulation circuits such that the output of U14101 opens, the
positive hot supply is placed on Q14103-E. Output current is now stopped only by the
overvoltage/overcurrent protection provided by R14108, which is acting as a current
monitor for the output device.
If the failure mode shorts U14101 output or places it in a low impedance mode, the
negative hot supply, only limited by R14112 appears on U14101-C and thus Q14103-E.
It now takes very little output current to trip the latch and remove output drive. All
supplies will be reduced and not maintain any regulation.
TECH
TIP
Precision Shunt Regulator
The three terminal precision shunt regulators used throughout the various supplies
of the CTC203 are unique devices. They may be thought of as "gated" zener
diodes, or infinite gain operational amplifiers with a reference voltage tied to the
negative input. In both cases, for the CTC203 chassis, 2.5V is the reference
voltage.
Figure A shows the regulator when the reference voltage on pin 1 is above 2.5V. The
regulator conducts, its internal impedance decreases, and current through the device
increases.
Figure B shows the regulator when the reference voltage on pin 1 is less than 2.5V. The
internal impedance of the regulator increases and current flow through the device
decreases.
In both cases, the current through the regulator directly drives the LED side of the
opto-isolator. As this current increases, the output impedance of the opto decreases.
As current decreases, the output impedance increases.
U14101
U14102
R14116
2000
0.1%
R14115
143K
0.1%
+16Vs
Reg B+
1
2
3
>2.5
Decreased
Internal
Impedance
Increased
Current Flow
U14101
U14102
R14116
2000
0.1%
R14115
143K
0.1%
+16Vs
Reg B+
1
2
3
< 2.5
Increased
Internal
Impedance
Decreasing
Current Flow
Figure A Figure B
26 Power Supply
Run Mode
In order to supply the different current demands between standby and run modes, the
main supply monitors the +13Vr supply generated from scan. If the supply is
running, Q14107 is on, turning off Q14106. This removes R14126 from the
regulator circuit and supply operates normally.
When scan is lost, the +13Vr supply is removed turning off Q14107. This turns on
Q14106 placing R14126 in parallel with the second regulator network resistor
R14116. This effectively lowers the resistance of the pair. It takes less Reg B+
voltage to trip the latch and current in the output transformer is decreased.
Figure 2-16, Run Mode
Neg Hot
Bias Supply
Pos Hot
Bias Supply
Q14107
Q14106
R14126
37.4K
CR14111
R14115
143K
R14116
2000
R14127
10K
R14113
1300
R14111
10K
R14112
680
R14128
680K
U14101
+13Vr U14102
+16Vs
+16Vs
Reg B+
CR14117
16V
To Control
Q14103-E
For instance, during normal operation, only R14116 and R14115 are in the feedback
voltage divider. If Reg B+ increases, the sample voltage at the gate of U14102
increases, output current decreases and Reg B+ begins to fall. If it falls such that the
voltage divider drops below the expected voltage level, output current is increased to
raise Reg B+.
When the set is in standby mode, the load on the secondary supply is greatly reduced
and Reg B+ tends to increase beyond the supplies ability to properly regulate it. By
placing R14126 in parallel with R14116 Reg B+ can go considerably higher than its
design while the sample voltage at U14102 remains the same.
The result is Reg B+ is allowed to be higher than normal by a fixed percentage based
on the parallel resistance of R14126 & R14116. That same percentage applies to the
remainder of the secondary voltages, but since the percentage is small, their regulation
will not be greatly affected. Reg B+ is not used during standby so it may be allowed
to float considerably above its required voltage. In effect, the parallel resistance
raises the target voltage (Reg B+) being regulated.
Power Supply 27
+12Vr
+9Vr
+7.6Vr
R14159
47
CR14115
5.6
U14104
+12V REG 1 3
2
U14150
+7.6V REG 1 2
3
R14123
470
1W
R14121
1000
R14156
51
1/2W
R14151
8.2
1W
CR14116
9.1
ONOFF
From Micro
U13101-19
Q14105
Q14104
+16Vs
+5Vr
+3.3Vr
Q14115
R14157
75
1/2W
C14118
10uF
U18101
+3.3V REG 3 2
1
RUN: High
Standby: Low
Figure 2-17, Run Supplies
Run Supplies
There are several supplies generated from the main supply but only required during
run operation. They are shown in figure 2-17. To turn them on and off System
Control sends a high to Q14105-B turning it on. That turns Q14104 on passing the
+16Vs supply to the input of the main +12V regulator. The output of the regulator
then feeds +12V directly to the circuits or feeds other regulators.
28 Power Supply
+200Vr
+23Vr
T14401
FOCUS
SCREEN
To Beam
Limiter
4
10
1/2W 20%
R14701
High Voltage TO
CRT ANODE
TO
CRT FOCUS
GRID
TO
CRT SCREEN
GRID
+13Vr
TO
CRT
FILAMENT
C14703+
47uF
250V
R14702
130K
1/2W
CR14702
R14509
300
2W
10%
R14703
0.88(0.82)
3W
R14508
1.0
CR14701 2W 10%
CR14704
9
8
5
7
10
6
2
Figure 2-18, Scan Derived Supplies
Scan Derived Supplies
Several other sources of power must also be generated by the CTC203. They are
derived from the scan circuits in a traditional way. Horizontal scan operation will be
covered later.
Two low voltage supplies are generated; +23V and +13V. An AC filament supply
for the CRT is taken from the same winding.
The CRT drivers require a higher voltage than can be generated by the normal
supply. It is generated here and is about +200V. It is slightly unique as it is derived
from the primary windings of the horizontal output transformer, not the secondary.
The remainder of the scan derived supplies are used to power and control the CRT.
They are the anode, focus grid and the screen grid supply.
Power Supply 29
When output MOSFET Q14101 fails, it is a good idea to replace the latch transistors,
Q14102 & Q14103. Unexpected excessive current may damage these transistors
and other components in the immediate area.
TECH
TIP
T14101
9
5
16
14
15
13
10
11
12
Q14102
Q14101
Q14103
3
8
R14107
43
R14106
2000
C14101
2.2uF CR14110
CR14106
CR14108
C14122
33uF
C14122
33uF
CR14107
33V
C14121
3.3uF
C14114
3.3uF
L14102
R14124
3.3
2W
Reg B+
R14109
750
R14110
22K
C14108
0.047
C14104
0.047
CR14103
CR14104
R14108
0.1
3W
R11513
4700
CR11504
18V
Q11501
R14103
1Meg
R14104
3300
R14101
47K
R14102
6800
CR14101
47V
CR14102
CR14105
C14108
1100
1.6KV
RAW B+
Neg Hot
Bias Supply
Neg Hot
Bias Supply
Pos Hot
Bias Supply
Pos Hot
Bias Supply
R14105
10
R14113
1300
R14112
680
U14101
U14102
+16Vs
CR14117
16V
+33Vs
+16Vs
+7.6Vs
+5.2Vs
-12Vs
-12Vr
CR11505
NC
U14103
+5.2V
Reg
+12VrSW
-12V
Fil
C14116
R141111 47uF
10K
Q14107
Q14106
R14126
37.4K
CR14111
R14115
143K
R14116
2000
R14127
10K
R14128
680K
+13Vr
+16Vs
RegB+Vs
Figure 2-19, Main Power Supply (Repeated)
Replace all on any
Output Device
Failure
30 Deflection
Deflection Overview
The CTC203 deflection circuits are very similar to previous TCE core line chassis.
Some models will have pin-corrected yokes, while others use an active pincushion
correction circuit. XRP is the same as previous chassis and other CRT control and
protection is also similar.
The horizontal deflection system has two primary functions in the CTC203 chassis.
First, it supplies the current for the horizontal yoke coils providing energy necessary
to move the electron beam horizontally across the face of the picture tube. Second,
it provides a number of voltage supplies needed for operation of the CRT and
deflection.
Horizontal yoke current is provided by a circuit consisting of a switch (HOT), the
primary inductance of the Integrated High Voltage Transformer (IHVT), a retrace
capacitor, trace capacitor (S-Shaping capacitor), and the horizontal yoke coils.
Voltage supplies provided by the horizontal deflection system are derived from
secondary and tertiary windings on the IHVT. The supplies are used by the video
amplifier (kine drivers), tuner, CRT, and the vertical amplifier.
Low level signal processing circuits for the horizontal deflection system are contained
in the T4-Chip. These include the horizontal sync separator and a two-loop horizontal
AFPC system. The T4-Chip allows bus control of several parameters associated
with the horizontal deflection system. These include horizontal drive pulse width,
AFC Gain, Sync Kill, and ON/OFF.
Enabling or disabling the horizontal drive signal from the T4-Chip determines
whether the chassis operates in the Standby or Run mode. In the Standby mode, no
IHVT-derived supplies are present reducing standby power requirements.
The vertical deflection circuit in the CTC203 is a linear amplifier DC coupled to the
vertical yoke coils. The circuit is similar to the CTC197 vertical circuitry. The
vertical ramp is generated in the T4-Chip. Vertical size, bias, S-Correction, and
linearity adjustments are done in the T4-Chip via the IIC bus. Timing information
for the ramp generator is derived from a digital vertical countdown circuit, resulting
in excellent interlace performance. The vertical output stage includes an integrated
circuit containing the power amplifier, vertical flyback generator, and thermal
protection.
Deflection 31
Deflection Basics
This discussion will only touch on horizontal, (right-left, left-right) deflection of the
electron beam across the face of the CRT. Vertical, (up/down, down/up), deflection
occurs in a similar fashion, just a different direction on the screen.
Although there is only one horizontal yoke winding, it is wound in such a fashion
that current in one direction drives the beam away from center to the left side of the
screen, while current in the opposite direction drives the beam away from center to
the right side of the screen. The strength of the current determines how far from the
center the beam is deflected.
Deflection is accomplished by forcing current through the deflection yoke, creating
an electromagnet from the yoke windings that either push the electron beam away
from or allow it to drift back to the center of the screen. If there is no yoke current,
the beam remains center screen creating a vertical line very close to the physical
center of the CRT. Figure 3-1 and 3-2 show the electron beam position at various
yoke current values, assuming a static DC current from a power supply is used.
(These values are only for discussion and demonstration purposes. Actual yoke
current and direction for exact beam positioning will be different.) Note that as yoke
current increases towards a higher positive
value, the beam is driven farther towards
the right side of the screen. As the
positive yoke current approaches zero,
the beam is closer and closer to center
screen.
Center of
Screen
Electron
Beam Position
+2A +4A +6A +8A +10A
Figure 3-1, Electron Beam Position with Positive Current
Center of
Screen
Electron
Beam Position
-10A -8A -6A -4A -2A
Figure 3-2, Electron Beam Position with Negative Current
As yoke current reverses, the
beam is again driven away from
center screen, but now in the
opposite direction. The higher
the negative current, the farther
from center screen the beam is
driven. As negative current
decreases, the beam moves
back towards center screen.
32 Deflection
Center of
Screen
+Max
-Max
Zero
Decreasing Yoke
Current Now
Allows Beam
To Move Back
To Center from Right
Electron
Beam Travel
+Max
-Max
Zero
Center of
Screen
Yoke Current now
Reverses and Begins
Increasing, Driving
Beam to Left Side
of Screen
Electron
Beam Travel
+Max
-Max
Zero
Center of
Screen
Decreasing Yoke
Current Again
Allows Beam
To Move Back
To Center from Left
Electron
Beam Travel
Center of
Screen
+Max
-Max
Zero
Increasing Yoke Current
Drives Beam
Away from Center
To Right Side
of Screen
Electron
Beam Travel
Figure 3-3 shows how increasing positive current drives the electron beam towards the right
side of the screen and increasing negative current drives the beam towards the left side. The
amplitude of current drives the beam farther from center screen. (The scope captures are not in
exact time alignment with the electron beam.)
Again, the theory of positive and negative current flow is not important to this discussion. The
concept of yoke current flow one way making the beam travel one direction, while yoke
current flow in the opposite direction makes the beam reverse its travel is the point.
Figure 3-3, Beam Travel
Inductive Current Flow
Among the many theories of deflection, yoke current versus yoke voltage is one of the most misunderstood
by technicians. A yoke is simply an inductor constructed to induce its developed magnetic flux in a
specific pattern around the bell of a CRT. The flux becomes stronger as current through the wire is
increased, and weaker as it decreases. Figure 3-4 compares voltage across a yoke winding with the
resulting current through it and magnetic field developed by it.
As voltage is first applied, the yoke tends to "limit" current flow. Even though maximum voltage is
immediately available, current builds slower as a result of inductive reactance. As current builds,
magnetic flux fields emanating from the yoke grow
stronger.
When voltage is removed, the yoke tends to continue
current flow as the flux fields (with no current flow to
sustain them) begin to collapse. As they collapse,
current decreases and the magnetic field grows weaker.
If voltage is not reapplied, the current will fall to zero.
The yoke is not directional. If the opposite polarity
voltage is applied, the same current pattern is observed,
only in the opposite direction.
Time
Volts
Current
Flux
Strength
0
0
0
Yoke
Winding
Voltage
Figure 3-4, Yoke Current versus Applied Voltage
Deflection 33
19
38 Phase
Detector
Loop
Filter
32 fH
VCO
Divide
by 2
2nd AFC
Ramp
Generator
Horizontal
Phase
Duty Cycle
Control
Horizontal
Drive
Horizontal
Output
H Lock
Detector
To Countdown
Circuits
Y IN
Part of T4 Chip
U12101
24
23
22 Horizontal Output
Flyback Pulse
X-ray Protect
Horizontal
Ground
21 Horizontal
AFC Filter
Divide
by 16
Sync
Separator
Figure 3-5, T4-Chip Horizontal Deflection
Low Level Horizontal Deflection
The T4-Chip employs a two loop horizontal AFC system. The first loop is used to
lock an internal 1H clock to the incoming horizontal sync signal derived from the
baseband luma signal. The second loop is used to lock the 1H clock to a feedback
pulse derived from a secondary winding on the IHVT. As with the other T-Chip
versions, a horizontal to video phase control is available via the IIC bus. The phase
control can be used as a horizontal centering control during alignment.
The first loop employs a 32H (32 times the horizontal frequency) VCO referenced to
a 503 kHz ceramic resonator.
The output at U12101-22 is shown.
Figure 3-6, U12101-22 Output Waveform
34 Horizontal Deflection
Low Level Signal Generation
The low level horizontal waveform generated from the T4-Chip has all correction
signals added prior to the output from U12101-22.
The horizontal driver circuit serves as an interface between the low level horizontal
output of the T4-Chip and the high power horizontal output circuit. The driver operates
in a "flyback" configuration storing energy driver transformer, T14301, during the
conduction cycle of Q14301. When Q14301 turns off, stored energy is dumped into the
base of Q14401, the horizontal output transistor (HOT). A buffer stage has been added
to reduce the amount of current that must be handled by the T4-Chip horizontal output
stage. This buffer consists of Q14302 and its associated circuitry.
The horizontal drive waveform app
|
FORUM
SEARCH
WHO'S 
LOG 
RULES
1
