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To convert fs to seconds: multiply by 10⁻¹⁵. To convert fs to picoseconds: divide by 1,000.
1 fs = 10⁻¹⁵ s = 0.001 ps = 1,000 as. Light travels about 0.3 µm in one femtosecond.
For example, 1 Femtosecond (fs) = 1.002738e-15 Second (Sidereal) (s (Sid)).
| Femtosecond (fs) | Second (Sidereal) (s (Sid)) |
|---|---|
| 0.1 | 1.002738e-16 |
| 0.5 | 5.013689e-16 |
| 1 | 1.002738e-15 |
| 2 | 2.005476e-15 |
| 5 | 5.013689e-15 |
| 10 | 1.002738e-14 |
| 25 | 2.506845e-14 |
| 50 | 5.013689e-14 |
| 100 | 1.002738e-13 |
| 500 | 5.013689e-13 |
| 1000 | 1.002738e-12 |
The femtosecond is a unit of time equal to 10⁻¹⁵ seconds — one quadrillionth of a second.
1 fs = 10⁻¹⁵ s = 0.001 ps = 1,000 as. Light travels about 0.3 µm in one femtosecond.
To convert fs to seconds: multiply by 10⁻¹⁵. To convert fs to picoseconds: divide by 1,000.
LASIK eye surgery uses femtosecond lasers. Also used in precision micro-machining and optical frequency combs.
A femtosecond is to one second as one second is to about 31.7 million years. The fastest chemical reactions occur on femtosecond timescales.
Confusing femtoseconds with picoseconds. Remember: fs is 1,000× shorter than ps.
Ahmed Zewail's Nobel-winning work proved we can 'photograph' chemical reactions happening in femtoseconds using ultrafast laser pulses.
The sidereal second is 1/60 of a sidereal minute — approximately 0.99727 solar seconds.
1 sidereal second ≈ 0.99727 solar seconds. 86,400 sidereal seconds = 1 sidereal day.
To convert sidereal seconds to solar seconds: multiply by 0.99727. One solar second ≈ 1.00274 sidereal seconds.
Telescope tracking motors rotate at sidereal rate (1 revolution per sidereal day) to follow stars across the sky.
The difference between sidereal and solar seconds (2.73 ms) seems tiny, but over a day it adds up to the full ~236 s difference.
Assuming sidereal seconds equal solar seconds. The ~0.27% difference is critical in precision astronomy.
Multiply any sidereal time interval by 0.99727 to get the solar equivalent. This ratio stays constant at all time scales.



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