Laser Selector
Tuloksen yhteenveto
| Kohde | Arvo | Yksikkö | Huomautukset |
|---|
Kaava
Rajat ja oletukset
Yllä olevaan kaavaan perustuva insinööriarvio. Varmista valitut osat ajantasaisesta datalehdestä ja järjestelmän toleransseista ennen tuotantoa.
Laserin perusteet
Hetkellinen huipputeho pulssienergian ja pulssin leveyden perusteella.
Jokainen luku luetaan kyseisen osan tietolehtisyötöstä ja muunnetaan kentän pyytämäksi yksiköksi.
Linkki avaa saman laskentakohteen ja samat syöttöarvot. Tiliä ei tarvita.
Raportti sisältää syötteet, yksiköt, tuloksen, kaavan, rajat ja sopivat osat.
PDF avaa tulostusikkunan; valitse Tallenna PDF-tiedostona.
Piirretty yllä olevista arvoista, piirretty uudelleen kirjoittaessasi - sama fyysinen kaavio, jonka miniohjelma näyttää.
Calculation guide
Peak power is the highest optical power during a pulse. This calculator converts pulse energy and an equivalent pulse duration, then lets you solve for any one of the three quantities.
P_peak = E / τ_eff
Use an equivalent rectangular duration. Fill E in mJ and τ_eff in ns, then P_peak is returned in W.
P_peak[W] = E[mJ] / τ_eff[ns] × 10^6
The 10^6 factor combines the mJ-to-J and ns-to-s conversions.
P_peak ≈ 0.939 × E / τ_FWHM
For an optical-power envelope with a Gaussian shape. A sech² pulse uses approximately 0.881 instead.
| Muuttujat ja yksiköt | Yksikkö | Huomautukset |
|---|---|---|
| Pulse energy E | mJ | 1 mJ = 10^-3 J; 10 µJ = 0.01 mJ. |
| Pulse width τ | ns | 1 ns = 10^-9 s. Enter the energy-equivalent rectangular width, not an arbitrary visible width. |
| Peak power P | W | 1 W = 1 J/s. This is optical peak power, not pulsed electrical current. |
E = 10 µJ, τ_eff = 100 ns → P_peak = 0.01 / 100 × 10^6 = 100 W
These are the nominal values of PLD905-100W-M at 100 ns.
P_peak = 100 W, τ_eff = 100 ns → E = 100 × 100 × 10^-6 = 0.01 mJ
The round trip returns 10 µJ.
E = 10 µJ, τ_FWHM = 100 ns → P_peak ≈ 0.939 × 100 = 93.9 W
Use the waveform correction when the datasheet specifies a Gaussian FWHM instead of an equivalent rectangular width.
The base formula assumes a rectangular pulse. FWHM is not the same as the energy-equivalent duration; convert it first or apply the shape factor shown above.
Peak power cannot be raised by shortening a pulse without considering current, duty cycle, junction heating and the diode's safe operating area. The PLD905 standard family quotes 1–100 ns pulses and 0.1% maximum duty cycle; confirm the exact model and bin.
Duty = τ × f_rep. At 100 ns, a 0.1% limit caps repetition rate at 10 kHz. Average power is P_avg = E × f_rep; verify it separately against the thermal budget.
Datasheet pulse energy is usually stated at a defined current, width and temperature. Do not assume that peak power or energy scales linearly outside that point.
Driver rise time, ringing, overshoot, optical losses and detector bandwidth all change the measured result. Use a calibrated optical waveform and integrate energy over the full pulse.
Peak power, average power, wavelength and pulse duration all enter the laser-safety assessment. Keep the system inside its declared laser class and applicable standards.
Representative catalogue routes for comparing rated peak power, pulse energy and pulse duration. The live recommendation list above is filtered by the values currently entered.
Compact TO56 starting point for short-range ranging and LiDAR.
Matches the default worked example and is useful for a direct calculation check.
Six-emitter part for longer-range ranging and time-of-flight systems.
Higher-power nine-emitter option; check thermal design and driver current.
Cross-check: the same equivalent rectangular calculation gives about 8 kW for 40 µJ in 5 ns.
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