A field team faces an unresolved physical question: Will the tag still wake when the coin cell is cold? They must answer it before changing pulse current on the real device. Predict the direction first.
See the relationship before changing it
The figure reads from left to right. The blue card is pulse current. The middle card applies this page's relationship. The green card is nameplate energy. Walk the arrows once: set the input, apply the rule, then read the result with its unit.
The retained audit below checks several chapter fixtures. This added model holds every other chapter fixture fixed, so the numeric fixture does not switch without explanation.
Derive the baseline in four named moves
- 1
Name the input. The chapter baseline for pulse current is 15.
- 2
Name the relationship. E = 0.225 x 3 = 0.675 Wh Qusable = 225 x 0.99² x 0.85 = 187.4 mAh Iavg = 187.4 Ah / 17,520 h = 10.7 uA Vcold = 3 - 0.015 x 60 = 2.10 V
- 3
Substitute the chapter fixture. Set pulse current to 15. The page ledger gives nameplate energy as 0.675 Wh.
- 4
Read the result. Keep Wh beside the value. Use it only inside the technical boundary on this page.
Predict, then change pulse current
Try Predict the direction of nameplate energy. Move one control, calculate, then check your prediction.
Observe The same pulse current produces three times the sag when internal resistance triples. Reset the control to 15 and compare nameplate energy.
Explain Only pulse current moves here. The other chapter fixtures remain fixed.
Check yourself
What should you do before trusting a moved-control result?
What does this small model leave out?
1. Start with the physical story
A BAP tag can have charge left yet reset during a brief cold pulse because internal resistance turns current into voltage sag.
2. Name every algebra move
Convert chargeUse E = QV for nameplate watt-hours.
Derate timeCompound self-discharge, then reserve cutoff headroom.
AverageDivide usable mAh by the 24-month hours.
Load the cellUse Vterm = Voc − IR for warm and cold resistance.
3. Reproduce the chapter case
Qusable = 225 × 0.99² × 0.85 = 187.4 mAh
Iavg = 187.4 Ah / 17,520 h = 10.7 µA
Vcold = 3 − 0.015 × 60 = 2.10 V
The arithmetic explains why a warm bench read cannot stand in for the refrigerated pulse test.
4. Try one real input
TryMove pulse current while capacity, service interval, and the two resistance screens stay fixed.
ObserveAt 15 mA the warm model keeps 0.70 V above cutoff, while the cold model keeps only 0.10 V.
ExplainThe same pulse current produces three times the sag when internal resistance triples.
This is a constant-resistance pulse screen, not a cell discharge simulation.
- Cell data
- Resistance, capacity, and cutoff vary with part, temperature, state of charge, pulse length, and ageing.
- Load
- Sensing, logging, leakage, regulator loss, and reader-field effects need measured duty traces.
- Fleet
- The replacement rate is a planning average, not a failure-time distribution.
Correct, not complete: this ledger does not approve a cell or predict tag life.
5. Use the result in the lab
Replay the measured pulse at warm and cold limits, log the cell terminals at the tag, and check reset and data retention.
6. Record the evidence state
Keep cell lot, age, temperature, pulse trace, cutoff, tag firmware, load profile, failures, and retest trigger.
7. Check yourself
Does 187 mAh prove two years of service?
Why can a cell with charge left still reset?
Does the monthly replacement average predict each failure?
The ledger converts explicit chapter constants into a benchable cold-pulse hypothesis.
- Computed
- Charge derating, average budget, sag, terminal voltage, and cutoff headroom are reproducible.
- Specified
- The selected cell's temperature curves and tag cutoff replace the illustrative constants.
- Observed
- Oscilloscope traces, resets, read success, and retained logs decide the outcome.
Correct, not complete: test the real cell and tag across the claimed cold interval.
Eddie guides