Falling rock

How fast does a rock hit the ground after a 300 m fall?

You ask

How fast does a fist sized rock hit the ground after falling off a 300 m cliff?

Wobbl runs

Terminal
$ wobbl motion --name rock --diameter "9 cm" --density "2700 kg/m3" \  --cd 0.6 --height "300 m"

Modeled4 state variables

  • gravity falling off with altitude
  • 1976 standard atmosphere
  • air drag

Checks

  • passstep convergence
  • passhand calculation
  • passvacuum drop
  • passenergy balance
  • passunits and sanity

Events

EventTimeAltitudeSpeed
Release0 s300 m0 m/s
Impact8.72 s0 m56.8 m/s
Altitude from release to impact, with the same drop without air dashed.

OKHits the ground 8.72 s after release at 56.8 m/s (205 km/h). Without air it would land after 7.82 s at 76.7 m/s, so drag takes 26% off the impact speed.

Fall time
8.72 s
Impact speed
56.8 m/s
Without air
7.82 s, 76.7 m/s
Confidence
high
summary.txt
summary.txt
OK. Hits the ground 8.72 s after release at 56.8 m/s (205 km/h). Without air it would land after 7.82 s at 76.7 m/s, so drag takes 26% off the impact speed. Confidence: high. passed step convergence, hand calculation, vacuum drop, energy balance, units and sanityfall time: 8.72 simpact speed: 56.8 m/swithout air: 7.82 s, 76.7 m/sterminal speed: 66.2 m/s Checks:  [pass] step convergence: flown again with a tolerance ten times tighter, the flight time 8.72 s and impact speed 56.8 m/s moved by at most 1e-06% (the impact speed)  [pass] hand calculation: with the air at its density halfway down (1.207 kg/m3) the terminal speed is 66.2 m/s, and v = vt tanh(g t / vt) with h = vt^2/g ln cosh(g t / vt) gives 8.719 s and 56.9 m/s against 8.717 s and 56.8 m/s from the run (0.16% apart), the difference coming from the air thickening on the way down  [pass] vacuum drop: with the air taken away and gravity held at its ground value the run lands after 7.822 s at 76.7 m/s, and sqrt(2h/g) gives 7.822 s and 76.7 m/s (1.5e-13% apart). The air adds 0.895 s to the fall and takes 19.9 m/s off the impact  [pass] energy balance: drag took 1.37 kJ and gravity gave 3.03 kJ, which leaves 1.66 kJ of kinetic energy at impact, and the impact speed carries 1.66 kJ (apart by 4.9e-07% of the largest term)  [pass] units and sanity: speeds stay under Mach 0.167, 1.03 kg in a 9 cm body, 2700 kg/m3 for a sphere Assumptions:  - A point mass in a vertical plane, so it does not spin, tumble or move sideways, and its drag acts against the air rushing past it.  - Drag coefficient 0.6 on a frontal area 9 cm across, the same at every speed.  - The 1976 US standard atmosphere from 0 m above sea level, a standard day.  - Gravity falls off with the square of the distance to the Earth's center, over a flat Earth that does not rotate.  - Still air. Images: flight: images/flight.pngReport: report.html

Open the full report

About this example

This is the simplest thing Wobbl can simulate. A fist sized lump of granite, taken as a sphere 9 cm across at 2700 kg/m3 so it weighs 1.03 kg, drops from rest off the top of a 300 m cliff. A tumbling rock averages a drag coefficient of about 0.6 on its frontal area, and the air is the 1976 standard atmosphere, about 3% thinner at the top of the cliff than at its foot.

Result Value
Fall time 8.72 s, against 7.82 s without air
Impact speed 56.8 m/s (205 km/h), against 76.7 m/s without air
Terminal speed 66.2 m/s, which the rock never quite reaches
Hand calculation the quadratic drag solution, with the air’s density taken halfway down, gives 8.72 s and 56.9 m/s
Energy balance gravity gives 3.03 kJ and drag takes 1.37 kJ, which leaves the 1.66 kJ the impact speed carries
Altitude and speed over the fall, with the fall without air dashed

For the first two seconds the rock falls almost exactly as it would in a vacuum, because drag grows with the square of its speed. After that drag catches up, and by the ground it takes a quarter off the impact speed and adds nearly a second to the fall. The same run with the air taken away and gravity held at its ground value lands when sqrt(2h/g) says it should, agreeing to more than ten digits, and every number above held when the flight was integrated again with a tolerance ten times tighter.

The trajectory is in output/trajectory.csv, one row per moment of the fall with time, height, speed, acceleration, Mach number and dynamic pressure.

Run it yourself

Terminal
$ git clone https://github.com/sohan-bhat/wobbl$ cd wobbl/examples/falling-rock && ./run.sh

The part, the script and every output are in examples/falling-rock on GitHub.