A field team faces an unresolved physical question: How can the meter change the sleep cycle it is measuring? They must answer it before changing cycle time 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 cycle time. The middle card applies this page's relationship. The green card is cycle charge (mc). 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 cycle time is 1.
- 2
Name the relationship. Q=0.130x0.100+0.005x0.250+0.120x0.050+0.000010x900=0.02925 A·s T=900.4 s Iavg=0.02925/900.4=32.5 uA 20 log10(0.120/0.000010)=81.6 dB
- 3
Substitute the chapter fixture. Set cycle time to 1. The page ledger gives cycle charge (mc) as 29.25.
- 4
Read the result. Keep the stated output unit beside the value. Use it only inside the technical boundary on this page.
Predict, then change cycle time
Try Predict the direction of cycle charge (mc). Move one control, calculate, then check your prediction.
Observe The same Ohm's-law multiplication controls both outcomes. There is no free shunt value: sensitivity and burden trade against each other. Reset the control to 1 and compare cycle charge (mc).
Explain Only cycle time 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
Current tells us how quickly charge moves. A short, high-current radio burst and a long, tiny sleep current both matter. To compare them fairly, multiply each current by its time. That product is charge. A shunt meter adds a resistor to the supply path, so it also creates a voltage drop that the unmeasured device did not have.
2. Name every algebra move
Find charge in every stateMultiply each state current by its duration: Q=I×t.
Add the chargesQtotal is the sum of boot, warm-up, radio, and sleep charge.
Add the timesTtotal is one complete wake-to-wake cycle.
Divide charge by timeIavg=Qtotal/Ttotal.
Test the measurementVburden=I×Rshunt at both the smallest and largest currents.
Compare the extremes20 log10(Imax/Imin) expresses the current span in decibels.
3. Reproduce the chapter case
T=900.4 s
Iavg=0.02925/900.4=32.5 µA
20 log10(0.120/0.000010)=81.6 dB
At 10 Ω, sleep produces 100 µV, but the radio peak loses 1.20 V. At 1 Ω, the peak burden falls to 120 mV while sleep produces only 10 µV. That is why the chapter changes range between states.
4. Try one real input
TryMove the control and predict which outputs should change before reading them.
ObserveIncreasing the shunt makes the sleep signal easier to see, but it removes more voltage during the radio burst. Average current and dynamic range do not change because they belong to the workload, not the meter.
ExplainThe same Ohm's-law multiplication controls both outcomes. There is no free shunt value: sensitivity and burden trade against each other.
This is a small formula ledger, not a complete source qualification.
- Catalog currents
- The state currents are example values; measure the actual board.
- Meter bandwidth
- A slow meter may miss a short radio peak even with a safe shunt.
- Battery behaviour
- This ledger does not include cell resistance or regulator loss.
Correct, not complete: the ledger proves the arithmetic and the shunt trade-off, not field battery life.
5. Use the result in the design
Choose a safe high-current range first, capture the peak, then use a lower-current range for sleep. Join the records by state and calculate average current from charge, not from a casual screen average.
6. Record the evidence state
Keep the board, firmware, rail voltage, shunt or meter range, state currents, state times, sample rate, and any brownout or reset. A changed range is part of the evidence, not a hidden detail.
7. Check yourself
Why is the cycle 900.4 seconds, not 900?
Why can a larger shunt falsify the result?
Why not average the four current numbers directly?
The arithmetic uses the chapter's named or clearly labelled catalog-typical inputs.
- Catalog currents
- The state currents are example values; measure the actual board.
- Meter bandwidth
- A slow meter may miss a short radio peak even with a safe shunt.
- Battery behaviour
- This ledger does not include cell resistance or regulator loss.
Correct, not complete: the ledger proves the arithmetic and the shunt trade-off, not field battery life.
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