Understanding the Laureate™ 1/8 DIN Panel Meters for A-to-B Time Interval
The Laureate™ 1/8 DIN Panel Meters for A-to-B Time Interval can display pulse width or time delay between individual pulses to a resolution of 0.2 µs, or the average pulse width or average time delay between multiple pulses. Timing starts when a pulse is applied to Channel A (selectable positive or negative edge) and ends when a pulse is applied to Channel B (selectable positive or negative edge). For a single pulsed signal, the A and B inputs can be tied together — a positive or negative slope starts timing, and the opposite slope must stop it.
Timing Technique and Averaging
Timing is achieved by counting 5.5 MHz clock pulses. Multiple integral time intervals are averaged over a gate time selectable from 10 ms to 199.99 s, which also controls the display update time. Periodic timing interval is gate time plus 30 ms plus 0-2 time intervals. Time Before Zero Output is separately selectable from 10 ms to 199.99 s.
Display Resolution by Range
Time interval displays in seconds, milliseconds, or microseconds with 6-digit resolution: 1 ms resolution from 0-199.999s, 100 µs from 0-99.9999s, 10 µs from 0-9.99999s, 1 µs from 0-0.999999s, and 0.2 µs from 0-0.099999s. For times under 100 ms, resolution down to 0.2 µs can be achieved by applying a multiplier of 10, moving the decimal point one position, and averaging many time intervals.
Rate Based on 1/Time (Extended Only)
Highly accurate rate can be displayed by taking the inverse of time, with extensive arithmetic capabilities for engineering-unit display such as meters/sec. A pulse or switch closure initiates timing, another stops it, and multipliers scale the result to appropriate units for any time duration.
Real-World Applications
- Time Delay Measurement — for periodic pulses on A and B channels, time delays are measured down to 0.2 µs resolution from the rising or falling edge of A to the rising or falling edge of B (selectable).
- Pulse Width Measurement — the width of periodic pulses is measured by tying A and B channels together, with readings averaged over a user-selectable gate time.
- Timing Process Dynamics — start/stop pulses generated by a dual relay board as a process variable passes two alarm setpoints or cycles in hysteresis control mode.
- Replacing an Oscilloscope — for fixed installations needing digital timing accuracy and control outputs rather than lab-bench viewing, a low-cost time interval meter with 0.2 µs resolution is the instrument of choice.
- Instrumenting a Pulsed Laser System — dual-channel counters provide elapsed time, pulse count, pulse width, pulse separation, duty cycle, and pulse repetition rate.
Factory-Calibrated Accuracy
Time base is crystal-calibrated to ±2 ppm, with ±1 ppm/°C span tempco and ±5 ppm/year long-term drift. Factory recalibration is recommended annually.
Where Time Interval Panel Meters Are Used
- Laser & Photonics Pulse Characterization — width, separation, and repetition rate measurement for pulsed laser systems.
- Delay Line & Propagation Timing — precise start-to-stop delay measurement between two independent trigger sources.
- Test Bench Replacement for Oscilloscopes — permanent, fixed-installation digital timing with control outputs.
- Process Dwell & Setpoint-Crossing Timing — interval measurement tied to relay-generated start/stop events.
- PWM & Pulse Width Verification — tied-channel pulse width measurement for signal quality checks.
- High-Speed Component Response Testing — relay, solenoid, and valve actuation-to-response timing.
- Rate-from-Time Velocity Measurement — inverse-time rate display for photodetector or switch-triggered speed sensing.
Time Interval Panel Meter Frequently Asked Questions
Why does the periodic timing interval formula include "0-2 time intervals" as a variable addition, rather than a fixed value?
This reflects the meter's need to complete at least one full, valid measurement cycle within the gate time window — since the timing interval being measured doesn't necessarily align perfectly with the start and end of the gate time, the meter may need to wait for up to two additional complete time intervals beyond the nominal gate time to ensure a complete, valid averaged reading before reporting the result.
How does the ×10 multiplier trick actually achieve 0.2 µs resolution for signals under 100 ms?
Documented guidance specifically describes applying a multiplier of 10 and moving the decimal point one position, combined with averaging many time intervals — this effectively displays a scaled, more finely resolved version of the underlying measurement by leveraging the averaging process across many cycles, extracting resolution finer than what a single raw measurement at that range would otherwise show on the display.
Does averaging multiple time intervals over a longer gate time improve accuracy, or just display stability?
Both, to different degrees — a longer gate time averaging more individual timing intervals reduces the random variation between individual readings (statistical averaging), which both stabilizes the displayed value and, for a genuinely stable and repetitive input signal, converges the average closer to the signal's true underlying interval, though it doesn't correct for systematic errors like a fixed trigger-level offset.
What's the difference between the "Time Before Zero Output" setting and the gate time setting?
Gate time controls how long the meter averages and how often it updates its reading, while Time Before Zero Output is documented as a separately selectable setting used specifically to indicate loss of signal — if no valid new pulse arrives within that configured window, the meter zeroes its output rather than continuing to display a stale prior reading indefinitely.
Can the same meter measure both a fixed delay between two separate signals and the pulse width of a single signal, or does it need reconfiguring for each?
Both modes are documented as available on the same hardware — the A-to-B delay measurement uses Channel A and Channel B connected to genuinely separate signals, while the pulse-width mode simply ties both channels to the same single signal — switching between these is a wiring and setup configuration change rather than requiring different hardware.
Why does the rate-based-on-1/time mode specifically require the Extended main board rather than being available on the Standard version?
Computing rate as the mathematical inverse of a measured time, along with the documented "extensive arithmetic capabilities" needed to scale that result into arbitrary engineering units, requires processing capability beyond simply displaying the raw timed interval — this is documented specifically as an Extended-board capability, consistent with the Extended board generally offering additional computational functions across the Laureate counter product line.
Does the laser instrumentation application's six listed parameters (elapsed time, pulse count, width, separation, duty cycle, rep rate) all come from reading the same physical pulse train?
Yes, potentially — the documented application specifically describes "some of the many possibilities" achievable from the same pulsed laser signal using dual-channel counters, meaning the underlying physical signal is the same across these measurements, though achieving several parameters truly simultaneously would typically mean configuring separate meters or channels, each set up for its own specific parameter, rather than one single reading yielding all six.
Is the maximum applied voltage rating the same across all input ranges, or does it vary by range like the resolution does?
It varies — documented specifications show maximum applied voltage at 600 Vac specifically for the 20V, 200V, and 300V ranges, but only 125 Vac for other ranges, alongside overcurrent protection that also varies by range (25x for 2 mA, 8x for 20 mA, 2.5x for 200 mA, 1x for 5A) — confirming the specific range in use against its own voltage and overcurrent rating matters rather than assuming one blanket protection level across all ranges.
Does choosing to display time interval in seconds versus milliseconds versus microseconds change the underlying measurement, or just the displayed units?
Just the displayed units and associated resolution — the underlying measurement is always based on the same 5.5 MHz clock counting technique, and the documented range-dependent resolution table (1 ms down to 0.2 µs) shows the display simply presents that same underlying count at whatever unit and decimal scaling is appropriate for the selected range, not a fundamentally different measurement process.
Can the A-to-B time interval mode measure a negative delay, where the Channel B pulse actually arrives before the Channel A pulse?
The documented timing mechanism specifically starts on a Channel A edge and stops on a Channel B edge — it's built around measuring the interval from a defined start event to a defined stop event, not around determining which of two independent, unordered pulses arrived first. An application where the physical B-triggering event could genuinely precede the A-triggering event would need the channels wired so that whichever event is expected to
Trigger-Level Timing Error & Slew Rate Questions From the Field
What is "trigger level timing error," and why does it matter for time interval measurements?
Documented metrology guidance specifically defines this as the timing uncertainty introduced when a signal's actual level at the moment of crossing the trigger threshold isn't perfectly known — because real trigger circuits have some uncertainty in the exact threshold voltage, and this voltage uncertainty translates into a timing uncertainty whose magnitude depends on how fast the signal is changing (its slew rate) at the trigger point.
How is trigger level timing error mathematically related to a signal's slew rate?
Documented formulas specifically express this relationship directly: timing error equals trigger level voltage error divided by the signal's slew rate at the trigger point — meaning for a fixed amount of trigger-level voltage uncertainty, a signal with a steeper (faster) slew rate at the crossing point produces proportionally less timing error than the same voltage uncertainty applied to a slower-rising or slower-falling signal.
Why is a square wave documented as having essentially zero trigger-level timing error compared to a sine wave?
A square wave's edges are documented as approaching infinite slew rate at the trigger crossing point, and since timing error is inversely proportional to slew rate, an infinitely fast transition drives the resulting timing error toward zero — a slower-transitioning signal like a sine wave crossing the same trigger threshold takes measurably longer to traverse the same voltage uncertainty band, producing a correspondingly larger timing error.
Does using a more sensitive trigger input setting always improve timing accuracy?
No — documented guidance specifically warns that increasing input circuit sensitivity can make trigger error worse rather than better, because a more sensitive threshold detector also becomes more susceptible to noise on the incoming signal causing the trigger point to fire too early or too late, which is a genuinely different error source (noise-driven trigger error) than the systematic trigger-level timing error tied to slew rate.
What's the documented difference between a "systematic" timing error and a "random" or noise-driven trigger error?
Documented distinctions specifically separate these: systematic error arises from consistent mismatches between measurement channels (such as differing rise/fall times or propagation delays between a start and stop channel), producing a repeatable offset that can potentially be calibrated out, while trigger/noise error is driven by genuinely random noise on the input signal and can't be removed through simple calibration since it varies unpredictably from measurement to measurement.
Is there a practical way to minimize trigger-level timing error without changing the input signal itself?
Yes — documented guidance specifically recommends triggering at the signal's offset value (the point of highest slew rate for a sine or square wave) specifically to minimize this error, and further notes that measuring from offset-to-offset (a full period or 0-degree phase reference between two signals) can cause hysteresis-window-related errors to cancel out, both being practical trigger-point choices rather than hardware changes.
Does averaging many time interval readings correct for trigger-level timing error the way it reduces random noise?
Not necessarily — documented distinctions specifically note that trigger-level timing error tied to slew rate is a systematic effect (the same bias applies consistently at a given trigger level and slew rate), so unlike genuinely random measurement noise, straightforward averaging across many readings won't cancel out a systematic trigger-level bias, since it's not actually random from measurement to measurement.
Do mismatched cable lengths or probe impedances between a start channel and stop channel genuinely introduce measurable timing error?
Yes — documented analysis specifically identifies mismatched probes, cables of differing length, and impedance mismatches between start and stop paths as real contributors to systematic timing error, with documented estimates showing meaningfully different error magnitudes depending on signal slew rate (a documented example shows roughly 70 ps of error for a slow-rising pulse versus only about 7 ps for a fast-rising pulse from the same impedance mismatch) — confirming matched cabling and impedances between channels genuinely matters for measurement accuracy.























Slide the meter into a 45 x 92 mm 1/8 DIN panel cutout. Ensure that the provided gasket is in place between the front of the panel and the back of the meter bezel.
The meter is secured by two pawls, each held by a screw, as illustrated. Turning each screw counterclockwise extends the pawl outward from the case and behind the panel. Turning each screw clockwise further tightens it against the panel to secure the meter. 






