A field team has a real problem to settle: Why does 499.2 MHz turn into a roughly 30 cm ranging floor? They must decide what happens before they change bandwidth on the device. Predict the direction first.
See the relationship first
The figure reads from left to right. The blue card is bandwidth. The middle card uses this page's rule. The green card is timing floor. Follow the arrows: set the input, use the rule, then read the result and its unit.
The audit later on checks more than one number. Here, the added model uses the baseline named below and holds every other chapter value fixed. That sentence bridges the fixtures, so the numbers do not change without a reason.
Derive the baseline in four moves
- 1
Name the input. The chapter baseline for bandwidth is 499.2.
- 2
Name the rule. Δt = 1/(499.2x10⁶) = 2.003 ns d = (3x10⁸ x 2.003x10⁻⁹)/2 = 0.3005 m At 20 MHz: Δt = 50 ns and d = 7.50 m
- 3
Put in the chapter value. Set bandwidth to 499.2. The page rule gives timing floor as 2.0 ns.
- 4
Read the result. Keep ns next to the value. Use it only within the limits on this page.
Predict, then change bandwidth
Try Predict what happens to timing floor. Move one control, calculate, then check your idea.
Observe Bandwidth buys timing detail. Exchanges can reduce random noise, but they cannot recover a pulse edge the channel filtered out. Reset to 499.2 and compare timing floor.
Explain Only bandwidth moves here. The other chapter values stay fixed.
Check yourself
What should you do before you trust the result?
What does this small model leave out?
1. Start with the physical story
A receiver cannot mark an edge more sharply than the channel preserves it. More bandwidth admits a shorter pulse, so the arrival-time window and the corresponding two-way distance window shrink together.
2. Name every algebra move
Invert bandwidthDivide one second by bandwidth to find the timing floor.
Convert unitsMultiply seconds by one billion to report nanoseconds.
Carry time into distanceMultiply by wave speed and divide by two for a round trip.
Compare screensDivide bandwidths and compare the range floor with the robot boundary.
3. Reproduce the chapter case
d = (3×10⁸ × 2.003×10⁻⁹)/2 = 0.3005 m
At 20 MHz: Δt = 50 ns and d = 7.50 m
The 0.3005 m screen reproduces the chapter's roughly 0.30 m result; implementation can be worse, never magically sharper than missing bandwidth.
4. Try one real input
TryMove occupied bandwidth and watch the same inverse relation drive timing, pulse length, and range resolution.
ObserveAt 499.2 MHz, the timing floor is 2.00 ns and the two-way range screen is 0.300 m, 24.96x sharper than the 20 MHz comparison.
ExplainBandwidth buys timing detail. Exchanges can reduce random noise, but they cannot recover a pulse edge the channel filtered out.
This is a bounded formula screen, not a deployment approval.
- Approximation
- 1/B is a physics-scale screen, not a complete correlator error model.
- Propagation
- Multipath and non-line-of-sight bias can dominate the nominal floor.
- Safety
- A 0.300 m screen does not certify a 0.25 m exclusion boundary.
Correct, not complete: use the measured state named above before release.
5. Use the result in the lab
Compare the screen with the required boundary, then measure bias and spread across line-of-sight and obstructed positions.
6. Record the evidence state
Keep channel, bandwidth, preamble and correlator settings, antenna delay calibration, geometry, reference distance, bias, and spread.
7. Check yourself
Does more exchange averaging beat the 1/B floor?
Why divide by two in the distance equation?
Does 499.2 MHz guarantee 30 cm accuracy?
The bridge keeps calculation, chosen inputs, and field evidence separate.
- Computed
- Timing floor, pulse length, two-way range screen, and comparison ratios.
- Specified
- Occupied bandwidth, wave speed, reference bandwidth, and robot boundary.
- Observed
- Bias, repeatability, first-path quality, and errors under real geometry and obstruction.
Correct, not complete: this page does not certify hardware, coverage, safety, capacity, or compliance.
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