
Average Blade Lift Coefficient Calculator
Calculate average blade lift coefficient for helicopter rotors with BEMT theory. Enter thrust coefficient and rotor solidity to get the dimensionless result.
Summer days near the Arctic stretch forever. Winter days barely make it past noon. Two numbers explain the difference: where you stand on Earth, and where Earth sits in its orbit. This calculator returns the theoretical maximum daylight at any latitude on any date. Solar designers, farmers, and astronomers all reach for the same figure when they plan around the sun.
Solar daylight hours (often written or N) is the number of hours the sun sits above the horizon at a given location on a given calendar day. It ignores atmospheric refraction and treats sunrise and sunset as the moments the sun's centre crosses a flat horizon, unlike civil or nautical twilight. That makes it the standard theoretical figure for estimating how much solar radiation reaches a site.
The value swings between extremes through the year. Near the equator, every day runs roughly 12 hours. Near the poles, daylight can stretch to a full 24 hours in summer or shrink to zero in winter. Earth's 23.45° axial tilt shapes the whole swing.
Enter your latitude in degrees, using a positive value for the Northern Hemisphere and a negative value for the Southern. Then enter the day of the year as a whole number from 1 (January 1) to 365 (or 366 in a leap year). You'll see the solar declination angle for that date and the daylight hours your location receives.
If you only know the calendar date, count the days: February 14 is day 45, June 21 is day 172, December 21 is day 355. The chart below plots daylight across the year at your latitude, so the chosen day's place in the seasonal swing is easy to read.
The maximum daylight hours are derived from the sunset hour angle:
Here φ is your latitude and δ is the solar declination, the angle between the sun's rays and Earth's equatorial plane. The 2/15 constant comes from rotation. Earth turns 360° in 24 hours, so 15° equals one hour. The factor of 2 covers both the morning and afternoon halves of daylight.
Declination itself depends on the day of the year (n):
Take London (φ = 51.5°) on June 21 (n = 172). At the summer solstice, . Then and , giving a product of 0.544. Apply the negative sign and take the arccosine: . Multiply by 2/15 and the answer is 16.39 hours, or roughly 16 hours and 23 minutes of daylight. That lines up with London's almanac on the longest day of the year.
Solar engineers treat as the upper bound on a panel's productive hours. Actual irradiance depends on weather and panel orientation, but no system can collect energy outside this envelope, so capacity planning, battery sizing, and payback math all start here.
Agriculture leans on it too. Long-day plants like spinach and lettuce flower once daylight crosses a critical threshold; short-day plants like soybeans stay vegetative until daylight drops back below it. Greenhouse growers add or remove supplemental lighting accordingly. Architects use for daylight harvesting, positioning windows and skylights to capture natural light. At high latitudes, where winter sun is in short supply, that planning matters most.
On the equinoxes (March 21 and September 23), δ = 0, so the formula collapses to 12 hours everywhere on Earth. That's the one date where latitude doesn't matter. Inside the polar circles (|φ| > 66.5°), the input to arccos can fall outside [−1, 1]. A value of −1 or below means the sun never sets, so daylight stays at 24 hours. A value of 1 or above means it never rises: polar night. The calculator clamps the input automatically, so you'll see 0 or 24 in those cases.
Not directly. is the time between geometric sunrise and sunset, when the sun's centre sits exactly on the horizon. Civil twilight adds roughly 30 minutes on top of that in temperate latitudes; nautical and astronomical twilight add more again.
Daylight duration depends on latitude and date, not on clocks. A time zone shifts when sunrise and sunset show up on your wall clock, but the gap between them stays the same.
Within a few minutes of true daylight in most cases. The Cooper equation used here ignores Earth's orbital eccentricity and the equation of time, so it can drift by up to about 15 minutes near the solstices. It's still the standard textbook approximation for solar engineering.
Enter latitude as a negative number. Sydney, for example, sits at roughly -33.9°. The formula handles both hemispheres, so the Southern summer (December solstice) returns the longest day there.
Indirectly. If you know solar noon for your longitude, sunrise is /2 before noon and sunset is /2 after. For exact clock times you'll also need the equation of time and your time-zone offset.

Calculate average blade lift coefficient for helicopter rotors with BEMT theory. Enter thrust coefficient and rotor solidity to get the dimensionless result.

Calculate aerodynamic drag force using the standard drag equation. Free tool for aircraft designers and engineers to analyze drag forces with velocity, air density, and wing area inputs.

Calculate aircraft pitching moment from moment coefficient, dynamic pressure, wing area, and chord length. Free aerodynamics calculator with interactive charts.

Calculate aircraft cruise range with the Breguet Range Equation. Enter cruise speed, TSFC, lift-to-drag ratio, and weights to solve for range or any variable.

Calculate jet engine thrust using the general thrust equation. Input mass flow rate, velocities, pressures, and nozzle area to determine net thrust force.

Calculate the pitching moment change from elevator deflection using the elevator power formula ΔC_M = C_M,δe · δe. Free online flight dynamics tool.
Solar Daylight Hours Calculator
Calculate maximum daylight hours for any latitude and day of year. Free solar daylight hours calculator with declination angle and formula explained.
https://hexacalculator.com/calculators/physics/engineering/solar-daylight-hours
Physics
Engineering