Before we go into the operation of the SLA Battery Charger schema, there are a number of points we need to cover about the care and use of Sealed Lead Acid batteries. The words Sealed Lead Acid covers a number of batteries that do not have a "filling hole."
You cannot get to the electrolyte and the battery can be used in any position. This discussion also covers AGM batteries (Absorbed Glass Mats) that have a separator between the plates and the electrolytic is thick and will not spill.
Another type: GEL CELL and FLOODED LEAD ACID all have the same or similar charging requirements and can be used with this charger because it is a low-current charger (about 300mA) and will not damage anything. It also has the feature of providing pulses to the battery when 13.4v is detected and this will eventually fully charge any battery and keep a it fully charged for months, and even years.
Firstly, Sealed Lead Acid batteries must be charged, discharged and stored very carefully. We normally think batteries can be stored for months (if not years) and they will be available for immediate use. This is not the case with SLA batteries.
If you store a NEW, full charged SLA battery for 6 months or more, you will find it may be fully discharged.
You may also find you cannot charge it!! It may be worthless. Thats how delicate SLA batteries are. They must be charged on a regular basis to prevent them discharging to a very low voltage level.
If the terminal voltage of a SLA battery is allowed to go below 8v, a process called SULPHATION starts to cover the surface of the plates and prevents the battery being re-charged. The internal resistance of the battery increases and it becomes useless.
HOW THE CIRCUIT WORKS
The schema consists of 5 building blocks: The schema does not turn on until a battery is connected across the terminals as shown in the diagram. (A push switch has been provided to start the schema when a totally flat battery is fitted.) This action turns on the PNP transistor in the "Turn ON" block. The resistance between the collector-emitter terminals decreases and the indicator LED comes on.
The path to the bottom rail of the schema goes through a signal diode, the gate-cathode junction of the SCR and through two 1R8 resistors in parallel. This is why the LED illuminates.
MUST USE AC PLUG PACKBefore we go any further, the schema works on an AC plug pack. It must be an AC supply as we do not want any electrolytics to be present on the power rail as this will allow a very high charge-current to flow and possibly damage the SCR. A DC supply will not allow the SCR to turn off, as it turns off when the current through it falls to zero.
THE CIRCUIT IS A HALF-WAVE RECTIFIER!The schema is actually a half-wave rectifier. It only charges the battery on every half cycle. The plug pack doesnt like this as it leaves residual flux in the core of the transformer and causes it to overheat. But thats the only drawback with the schema.
The SCR turns on during each half cycle and current flows into the battery. A voltage is developed across the two 1R8 resistors (in parallel) and this voltage is fed into the 47u electrolytic. It charges and turns on the BC547 transistor. The transistor robs the SCR of gate voltage and the SCR turns off. The energy in the 47u feeds into the transistor but after a short time it cannot keep the transistor turned on.
The transistor turns off and the SCR switches on and delivers another pulse of current to the battery. As the battery charges, its voltage increases and this is monitored by the "Voltage Monitor" block. The schema is very complex and one way to look at the operation is to consider the top rail as a fixed rail and as the battery voltage increases, the rail connected to the negative terminal of the battery is pushed down.
This lets you see how the "Turn On" transistor is activated and how the "Voltage Monitor" components create voltage drops across each of them. The "Voltage Monitor" components consist of a transistor and zener diode as well as an 8k2 resistor, the 1k pot, a 1k5 resistor, a 150R resistor and a signal diode. The signal diode is actually part of the flasher schema and we discuss its operation later.
As the voltage across the battery increases to 13.4 volts, each resistor in the "voltage detecting network" will have a voltage drop across it that corresponds to the resistance of the resistor. The diode will have a constant 0.7v across it. The voltage on the wiper of the pot will be about 3.25v and the voltage across the zener will be 10v. This leaves 0.6v between the base and emitter of the Voltage Monitor transistor.
This voltage is sufficient to turn the transistor ON.When the Voltage Monitor transistor turns ON, it robs the "Turn On" transistor of base-emitter voltage and the schema turns off.
The SCR has only two states: ON and OFF.During the half-cycle when it is turned on, the battery gets a high pulse of current and the current is only limited by the capability of the plug pack. There are no electrolytics to allow very high pulses of current to be delivered and this is fortunate as the SCR is only a 0.8 amp device, but will endure surges of 10amp for half a cycle.
Whenever the SCR is triggered into conduction during the half cycle of its operation, it remains in conduction until the voltage delivered by the plug pack falls to zero. This is when the SCR turns off. When the plug pack delivers a negative voltage to the top rail and a positive voltage to the lowest rail, the SCR is not triggered into conduction and none of the components in the schema deliver current to the battery. The SCR delivers current for a few half-cycles and then it is turned off for a few cycles. This is how the average current delivered to the battery is controlled.
The schema is designed to deliver about 300 - 400 mA average charge-current. The maximum value is determined by the 1R8 resistors. They do not allow any more than 900mA to flow during a half-cycle and if this current flows, the lower 47u is charged and the lower transistor turns on to prevent the SCR turning on.
When the battery is fully charged, the indicator LED begins to flash.
The flashing is produced by the 2k2 resistor and 47u (connected to the voltage monitor section). When the battery is charging, the 47u is charged via the diode connected to the BC557 transistor and through the 150R and signal diode to the negative of the battery.
When the battery is fully charged, the Voltage Monitor section turns ON and turns off the "Turn ON" section.
This removes the voltage on the positive side of the 47u and the positive side is brought to the negative rail via the 2k2 resistor. This brings down the negative side of the 47u and the 150R resistor is allowed to drop below the negative rail due to the presence of the diode, as the diode becomes reverse-biased.
This holds the schema in the "off" condition, as the voltage monitor section sees an extra voltage across it and thinks the battery it is "over-charged."
The 47u discharges and the schema turns ON to pump a small burst of current into the battery to keep it charged. This is called "Trickle Mode" or "Pulse Mode."
HOW TO SET THE POTCharge a battery and when the voltage reaches 13.4v, adjust the pot so the LED flashes.
DEAD BATTERIESThe schema will not turn on if the voltage of the battery you are charging is less than 4 volts. If you have a good battery that has been totally discharged, you can manually start the charging process by connecting the battery and pressing the button. This will raise the voltage on each cell and the schema will take over in the normal way once the voltage rises more than 4 volts.
SCR: MCR100
type - 6 400v
current 0.8A
Max current
for half cycle 10A
DONT WASTE YOUR TIMEIf you have a battery that does not charge, even after you have pressed the push button, dont waste your time. If it has been standing for more than 6 months in an uncharged state, it will not charge. This charger is ideal in determining if a battery is able to be charged.
Just connect it to the charger and monitor the voltage across the battery. If it remains at less than 8v after 1 hour, the battery is scrap. You can easily test a battery by putting a 12v car globe across the terminals. Even a tail light globe will require a current of more than 1 amp to get it to glow and if the battery cannot deliver this current, it is DEAD.
The only "dead" battery that can be recovered is one that has been connected to equipment and is totally exhausted. The equipment has exhausted the battery. If you charge it within a few weeks, the process of "sulphation" will not have damaged it and it can be fully charged. If the battery is "dead" due to standing for a long time, the chances of recovery are virtually nil.
Sealed BatteriesSealed batteries have the acid either gelled or put into a sponge-like glass mat. They have the advantage/disadvantage of being completely liquid-tight. They can operate in any position, even sideways or upside down, and will not leak acid. Because the electrolyte moves more slowly, these batteries cannot tolerate high rates of charging or discharging for extended periods, although their thinner plates will allow high rates for a short time. Their sealed construction, which makes them ideal for some limited applications, makes it impossible to check individual cell conditions with a hydrometer. Although these cells are "sealed," they do have vents to prevent pressure build-up in case of gassing. Many PV charge controls will push charging voltage too high for sealed batteries. Premature failure will result due to loss of water vapor. We recommend sealed batteries only in situations where hydrogen gassing during charging cannot be tolerated, or the battery is going to be moved and handled a great deal, or in conditions where the battery needs to fit into unique, tight spaces. Boats, UPS computer power supplies, and remote expeditions are the most common uses. Special lower voltage charge controls must be used with these batteries. Life expectancy is two to five years for most AGM (absorbed glass mat) batteries, and five to ten years for the higher quality, but more difficult to manufacture, gel cell batteries. Most sealed batteries are AGM types.
Here is a Printed Circuit board made by Tom Kelly, one of our readers:You can clearly see the track-work under the board and it is easy to copy the layout and produce your own board. The board was produced by Tom Kelly. You can email him for the file so you can make your own PC board.
Or you can buy a PCB from Talking Electronics with overlay and tinned solder-lands for $3.00 plus $3.00 postage
PARTS LIST
12v SLA Battery Charger
PCB $3.00 plus $3.00 post
2 - 1R8 0.5watt resistors
1 - 150R 0.25 watt resistor
1 - 180R
1 - 560R
1 - 1k5
3 - 2k2
1 - 3k3
1 - 4k7
1 - 8k2
1 - 1k mini trim pot
1 - 1n ceramic
2 - 47u 25v electrolytics
1 - 5mm red LED
4 - 1N4148 signal diodes
1 - 10v 0.25watt zener
1 - BC 547 transistor
2 - BC557 transistors
1 - MCR100-6 SCR
1 - 1m red lead
1 - 1m black lead
2 - alligator clips
1 - 2m very fine solder
1 - SLA Battery Charger PCB
Also required:
1 - 12v AC transformer (500mA AC)
1 - power lead
1 - case
Sourced by: talkingelectronics
D1 can work with as little as 10µA. The supply voltage for the IC is decoupled by R10, C3 and C4, with D4 providing over voltage protection. A maximum supply voltage of 16 V is specified for the TLC271. This opamp works with a supply voltage as low as 3 V and can handle a common-mode voltage up to approximately 1.5 V less than the positive supply voltage. Accordingly, 1.2 V has been chosen for the reference voltage. The fan voltage is reduced to the level of the reference voltage by the voltage divider R2–R3–P1. The limits now lie at 11.2 V and 16.7V.
If you find these values too high, you can reduce R2 to 100 kΩ, which will shift the limits to 9.5 V and 14.2 V. The output of the voltage divider is well decoupled by C2. A relatively large time constant was selected here to prevent the circuit from reacting too quickly, and to hold the output active for a bit longer after the comparator switches states. A small amount of hysteresis (around 1 mV) is added by R4 and R5, to prevent instability when the comparator switches. D2 ensures that the magnitude of the hysteresis is independent of the supply voltage. Two outputs have been provided to make the circuit more versatile.
Output ‘R’ is intended to directly drive the LED of an optocoupler. In addition, transistor T2 is switched on by the output of the opamp via R7 and R8, so that a relay can be actuated or a protection circuit triggered using the ‘T’ output. The high-efficiency LED D3 indicates that IC1 has switched. It can be used as a new ‘maximum’ temperature’ indicator when this circuit is added to the fan controller. The circuit draws only 0.25 mA when the LED is out, and the measured no-load current consumption (with a 12.5V supply voltage) is 2.7 mA when the LED is on.Resistors:
