Ramsey Doctor_NiCad_DN-1 User guide

N
i
Dr. NiCad
C
a d
BATTERY CONDITIONER/
RAPID CHARGER
Ramsey Electronics Model No. DN1
Stop shelling out a fortune on batteries ! Enjoy full performance from your NiCad batteries or battery packs with this sensational
Quick charges batteries for laptop computers, hand-held radios and scanners, cordless/cellular phones, camcorders, RC models and more ! Charge many batteries in less than an hour !
State-of-the-art battery monitor IC safely watches both battery voltage and charge time while fast charging your batteries !
Dr.Nicad is your best for nicad batteries!
R
x
Eliminate “Memory Effect” common to NiCads - uses unique constant current circuitry.
Safety First: circuit has “built in” timers and voltage sensors that monitor the cell for safety - it won’t let you charge a bad cell !
Stop “cooking” and start conditioning your rechargeable batteries, no more leaving the charger plugged in for days on end !
Charges single cells as well as NiCad packs from 1 to 10 cells !
Automatic “top off” charge keeps batteries at their peak power until
use.
Unit runs on 12-15 volts DC.
Convenient flashing LED indicates charging modes and eliminates
guesswork.
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RAMSEY MINI-KITS Many other kits are available for hobby, school, Scouts and just plain FUN. New kits are always under development. Write or call for our free Ramsey catalog.
DOCTOR NiCad BATTERY CONDITIONER KIT INSTRUCTION MANUAL
Ramsey Electronics publication No. MDN1 Revision 1.1a
First printing: March, 1994
COPYRIGHT
14564. All rights reserved. No portion of this publication may be copied or duplicated without the
written permission of Ramsey Electronics, Inc. Printed in the United States of America.
ã
1994 by Ramsey Electronics, Inc. 590 Fishers Station Drive, Victor, New York
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Ramsey Publication No. MDN1
Price $5.00
KIT ASSEMBLY
AND INSTRUCTION MANUAL FOR
Dr. NiCad NiCad BATTERY CHARGER/CONDITIONER
TABLE OF CONTENTS
Introduction to the DN1 ................. 4
How it works .................................. 6
Parts list ........................................ 8
Schematic diagram ....................... 9
Parts Layout diagram .................. 11
DN1 Assembly instructions ......... 12
Setup configurations .................... 16
Troubleshooting ........................... 21
Ramsey kit warranty .................... 23
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RAMSEY ELECTRONICS, INC.
590 Fishers Station Drive
Victor, New York 14564
Phone (585) 924-4560
Fax (585) 924-4555
www.ramseykits.com
INTRODUCTION
With today’s ever changing technologies, more appliances depend on battery power to enable their use. While this gives us greater freedom, it is often at the high cost of purchasing portable energy, or batteries, to run our portable electronic gismos. Consider the cost of energy from our local electric
company, about 8 penny. On the other hand, that 500 mA-H NiCad that you just purchased for about $1.75 can only supply 2250 joules of energy; that's about 13 joules for 1 cent. So it’s fairly easy to see that energy costs about 35,000 times more when it’s in a battery.
Nobody likes the idea of throwing all those batteries into a landfill. That's the reason for the recent emphasis on using “green” rechargeable cells. If a set of NiCad cells lasts you for a few months, they can save the equivalent volume of themselves many tens or hundred times in the trash. This is not only good for the environment, it’s also great for the wallet!
Nicad rechargeable batteries have been around for years, but there are a few real disadvantages in their use. They usually require a long time (sixteen hours) to recharge. This “trickle charge” arrangement is quite common because it is much cheaper for the original product manufacturer to produce (the entire battery charger is typically a couple of rectifier diodes and a current limiting resistor), and works well given the draw back of a long charge time.
Another disadvantage to the “plug-in wall transformer charger” is that the charging cutoff action is regulated by the heat produced by the cells’ chemical reaction when recharging. If you’ve ever opened up a rechargeable pack you have probably seen the thermal shutoff “mystery part” connected and mechanically touching one cell of the battery pack. While this will help if you leave your appliance charging for several days, notice that it is sampling only one cell in the pack, and assuming that the rest of the batteries are “behaving” in the the same manner. Also, since the ambient temperature can change (i.e.recharging your cordless drill in the cool garage or basement, or your two way radio on the hot seat in the car), this heat sensing approach can vary considerably from undercharging your pack to overcharging until you “cook” the electrolyte solution right out of the battery.
Often times we cannot wait for the full recommended charging time or do not use the batteries until they’re completely “dead”. When this is repeated, the uncared for battery or pack can seem to “run out” rather quickly. This effect is caused by not completely discharging the cell before it is recharged and is known as the memory effect, since the battery appears to memorize the amount of energy it is called upon to produce.. By not completing the
¢ for a KW hour, or about 450,000 joules of energy for a
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oxidation reduction or “redox" chemical reaction in the cell, we effectively decrease the chemically active surface area inside the cell. The lower this surface area, the shorter the battery’s life. Since you don’t try to recharge conventional batteries, you’ve never noticed this property until you started to use rechargeable NiCad batteries.
To keep your cells working like new and to eliminate this memory effect, we’ve built in an automatic discharge circuit that will properly discharge the cells before their recharging.
So, you can see recharging a NiCad battery correctly can be a tricky business. How can we charge the battery to its full potential, but not too much? The answer is to watch the V or change in voltage over time. As shown in the graph, the battery voltage continues to rise while charging but drops slightly when the cell is completely charged. By recognizing this point on the graph, a charger can put just enough charge into the cell. By virtue of this voltage -vs­time checking, it is also possible to charge the battery at a much higher charging current - and significantly reduce the battery charging time. Once this point is reached, it is best to “top off” the battery with a charge burst every now and then.
Positive "Slope" or + dV
dT
Full Charge
Slope = Zero
Negative "Slope"
or - dV
dT
Terminal Voltage vs Time for a NiCad Cell
VOLTAGE
TIME
Enter the Benchmarq BQ2003 NiCad battery charger IC. This cell monitoring / charging IC performs all of the previously mentioned functions, and then some. This smart IC is the “doctor” in our NiCad recharging unit.
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We designed our kit to change quickly and easily adapt to a variety of cell or battery pack types for anything from video camcorders to cordless phones. You can configure it for the number of batteries in your pack, discharge and charging rate. We’ll discuss this later as we’re assembling these sections of the circuit.
DN1 CIRCUIT DESCRIPTION
Before we get into the technical jargon, let’s take a walk around the BQ2003 Integrated Circuit . We’ll start with some definitions of the abbreviations written on the chip in the schematic diagram.
Benchmark BQ2003 pin designations:
Pin No. Abbreviation Function
1
2
3
4,5
7
8
9
11
13
14
15
16
CCMD Charge command
DCMD Discharge Before Charge Command
DVEN
- V Enable Input
TM1 & 2 Timer Mode Outputs
BAT Single Cell Voltage Input
VSS Ground
SNS Charging Current Sense Input
MCV Maximum Cell Voltage Reference
CHG Charging Status LED Output
MOD Current Switching Control Output
DIS Discharge Control Output
VCC 5 Volt input
The BQ2003 charger IC handles many of the functions related to our charger. Without trying to sound too much like a technical manual or data book, here’s a closer look at some of the accompanying circuitry. Have a glance at the schematic diagram and follow along.
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Since we want the voltage appearing at the IC to be equivalent to one cell, we first must “divide” the cell voltage by the number of cells in the pack. The ladder resistors R2 -R24 form an effective voltage divider circuit so that the BAT (pin 7) voltage will be about 1.25 V per cell. The switch can increase or decrease the BAT voltage by adding or subtracting “rungs” from the voltage divider ladder. Another divider network consists of resistors R14 and R16. This voltage sets up the MCV voltage for the BQ2003 IC. This should measure 1.8 V when in operation.
Seeing how you’ll want to charge your batteries quickly, you need a high charging current power supply to back you up. Transistors Q2, Q1, and components D1 and L1 form the “high current” portion of our “switched­mode-regulator” circuit. When the MOD output goes “high”, transistor Q2 is turned on, like a switch. This current then flows into the battery. Resistor R29 (and/or R27) is in series with the current flow and the voltage drop across it is sensed by IC pin 9, the sense pin. When the sense pin reaches its trigger point, the transistor is abruptly turned off. When this occurs, the magnetic field around the coil quickly collapses and causes a reverse voltage “spike” which is routed through the “catch” diode D1. This energy is recovered and delivered to the battery cells being charged. This is what provides us with the high current to quickly charge the cell, but does not dissipate power in the FET or NPN transistor, making the switched power much more efficient than a conventional pass transistor type of supply. Another contributing factor to the charging circuit is the charge rate setup, which is configured using resistors R26 and 27, as well as test points A - F.
Transistor Q3 is the integral part of our constant current discharging circuit. When the chip sees a positive going pulse at the DCMD pin, it initiates the DIS discharge output. With switch S1:10 closed diodes D2 and D4 are forward biased, causing 1.4VDC to be present at the base of Q3. With 1.4 V at the base, there is .7 VDC at the emitter, a diode drop in potential lost through the transistor. With the emitter at .7 VDC, the current through resistors R10 and R22 is about 140 mA, regardless of the cell voltages. If switch S1:10 is opened the potential increases to 1.4 VDC. increasing the current to 280 mA. This will continue to discharge the batteries until they reach a potential of about .9 volts per cell. The Benchmarq chip then initiates its own charging sequence.
A few final points concerning the TM1 and TM2 time-out, which are configured using points G - J. They are dependant on the charge capacity, or “C” of the pack. We’ll discuss this in more detail when it comes time to configure these jumpers.
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DN1 PARTS LIST
RESISTORS
1 270 ohm [red-violet-brown] (R12) 2 .5 ohm ½ Watt [green-black-silver] (R26, 27) 3 10 ohm [brown-black-black] (R 2, 10, 22) 2 470 ohm [yellow-violet-brown] (R3, 7) 4 1K ohm [brown-black-red] (R1, 5, 9, 25) 2 10K ohm [brown-black-orange] (R11, 20) 1 10K ohm 1% [brown-black-black-red] (R16) 1 17.8K ohm 1% [brown-violet-grey-red] (R14) 11 47K ohm resistors [yellow-violet-orange] (R4,6,8,13,15,17,18,19,21,
23, 24)
CAPACITORS
3 1uF electrolytic capacitors (C1,C3,C3A) 3 10 uF electrolytic capacitors (C2, 5, 6)
INDUCTORS
1 Axial lead inductor [enameled wire wound on ferrite core] (L1)
SEMICONDUCTORS AND INTEGRATED CIRCUITS
3 1N4148 diodes [glass case with black band] (D2, 4, 7) 2 1N4002 diode [epoxy case marked 1N4002] (D5, 6) 1 1N4937 fast recovery diode [ epoxy case marked 1N4937] (D1) 1 Light Emitting Diode [LED] (D3) 1 NPN small signal transistor [2N3904 or equivalent] (Q2) 1 NPN power type [marked TIP31C] (Q3) 1 Power FET [marked 7035] (Q1) 1 78L05 voltage regulator [marked 78L05] (VR1) 1 BQ2003 16 pin IC (U1)
MISCELLANEOUS PARTS AND HARDWARE
1 2.5mm power jack (J3) 1 10 position DIP switch (S1) 2 DPDT pushbutton switch (S2, 3) 1 DN1 printed circuit board 1 TO-220 heatsink (HS1) 2 #4-40 screws and nuts 1 Insulated jumper wire 1 6” piece of two conductive wire (blk, red)
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