The Alto de Patios climb from Usaquén, in Bogotá

Summary

Watts on Alto de Patios

Free calculator · Training and load

The power a target time on the Alto de Patios asks for, using the real air density of Bogotá at 2,600 m.

What you need
Your weight with the bike and the time you want to ride. The real gradient of the climb and the air density of Bogotá at 2,600 m are supplied by the calculator.
What it gives you

The average power that time asks for, with the air that actually exists at 2,600 m.

The watts per kilogram that means for you, which is the comparable figure.

How much the result changes if you change weight or position on the bike.

What it does not do

This is a physical model of the climb, not a prediction of the day: wind, traffic, the group and how you arrive all stay outside. And a calculated power is not a power you can hold.

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How many watts you need on the Alto de Patios

Enter the time you want to ride and it tells you the power to hold, or the other way around. It uses the real profile of the segment, taken from a GPX of the climb, and the air density of the pass — 2,653 to 3,019 m — which is 27 % lower than at sea level: any calculator that ignores that will lie to you here.

It runs in your browser. Nothing is sent, nothing is stored and no sign-up is needed. If you use the buttons below the calculator, the message is written here and opens in your own app: you decide whether to send it.

Calculator

You and your bike

Used to estimate your frontal area, which is what decides the drag.

It changes the position, the tyre and the state of the drivetrain, which is where the time goes. Picking one proposes a typical bike weight, which you can correct.

With bottles and everything you have fitted.

What the chain keeps between pedal and wheel. A dirty drivetrain costs more than a kilo of bike.

It multiplies your tyre's rolling resistance. It is one of the biggest gaps between the calculated time and the one on the clock.

It does not touch the physics: it moves the expected range, which is where the time lost braking and waiting to pass lives.

What you want to know
Target time

Minutes and seconds for the 5.9 km segment, from Belisario to the top.

How to spread those watts

All four spend the same energy: what changes is where you put it. Each time comes from solving the profile with that split and scaling the base power until all four add up to the same kilojoules.

Estimated time by power distribution
SplitTimeAgainst flat watts

The real profile, from the GPX

Run your finger or the mouse over it to read the kilometre, the altitude and the gradient at that point. With a keyboard: focus the profile and move with the arrow keys.

Kilometre

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Altitude

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Gradient

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Still to go

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Touch the profile to read a specific point.

012345km2,653 m3,019 m
Profile from the climb's GPX, one sample every 100 m. The vertical scale is exaggerated, as in any elevation chart: the climb gains 367 m over 5.9 km.

What changes the result

Sensitivity of the time to each variable
If you changeThe time

On a sustained ramp, weight rules over aerodynamics. That is why a kilogram counts for more here than on the flat, and why an aero position barely contributes.

The segment

  • 5,912 m from Belisario to the top, with 367 m of climbing and a 6.2 % average gradient.
  • Not one metre of rest: the hardest part is around 7.7 % near km 3.5 and the only relief drops to 2.7 % past km 4.6, but it never stops climbing.
  • From 2,653 to 3,019 m of altitude: air density of 0.89 kg/m³ against 1.225 at sea level.
  • It shares the profile, the air density and the base equation with the challenge simulator (in Spanish). The simulator adds the surface and the bike you choose, so its times are comparable but not identical.

Take the result with you

Send us this calculation and we will tell you what to do with it.

The button writes the message for you: what you entered, what came out and the name of the tool. It opens in your own app, already written, and you decide whether to send it. Nothing leaves this page until you do.

Your message opens ready to edit. Nothing is sent automatically.

Method and sources

References · 3 primary sourcesView the full citationsBassett et al. 1999 · Allen et al. 2019 · Böning et al. 2010

Primary sources and position statements the method on this page relies on.

  1. Bassett, D. R., Kyle, C. R., Passfield, L., Broker, J. P. and Burke, E. R. (1999). Comparing cycling world hour records, 1967-1996: modeling with empirical data. Medicine & Science in Sports & Exercise.
  2. Allen, H., Coggan, A. R. and McGregor, S. (2019). Training and racing with a power meter (3.ª edición). VeloPress.
  3. Böning, D. et al. (2010). Limiting factors of maximal oxygen uptake at altitude. High Altitude Medicine & Biology.

The cycling power equation is solved on every section of the profile: power is split between overcoming gravity, overcoming rolling resistance and overcoming the air.

Frontal area is estimated from your height and weight with the regression Bassett and colleagues (1999) built on the Du Bois body surface area, the usual procedure when there is no wind tunnel measurement. For a 176 cm, 72 kg rider it gives a CdA of about 0.33 m², the order of magnitude of riding on the hoods; the more upright position adds 8 %. Air density is0.89 kg/m³: what the pressure at the climb's mean altitude — 2,836 m — gives with the 9 °C of a morning on the plateau, not the sea level value. Using 1.225 here overestimates drag and with it the power required.

The profile comes from a GPX of the segment itself: 1,645 points with their elevation, summarised as the mean gradient of each 200 m block. Integrated in 20 m sections it returns the real 367 m of climbing, and that is how the time is calculated, not by applying an average gradient: between the 2.7 % of the relief and the 7.7 % of the hard part, the average lies.

The bike enters the equation, not as decoration

Three things about the bike change the result and here they are chosen one by one. The weight, which on a 6 % ramp weighs most. Thecomponent level, which sets the drivetrain's mechanical loss: 1.2 % with high end parts and up to 2.5 % with a dirty or worn chain. And the tyre, with rolling resistance from 0.0035 on a 25-28 mm racing tubeless to 0.0070 on a mixed gravel tyre. Picking your level is just a shortcut that fills all three with typical values; then you correct them.

On top of that comes the road surface, which multiplies rolling resistance and which almost no calculator asks about. It is not a detail: at 250 W, going from smooth asphalt to the patched surface this climb actually has costs around 25 seconds. That is why it defaults to “patched”, which is how the road is, and not to “smooth”, which is how the number looks prettier.

That mechanical loss was not there before, and it was why the model returned optimistic times. The power you type is pedal power — what your power meter reads — not what reaches the wheel.

What it is checked against

Against a Best Bike Split plan for this same segment with Egan Bernal's numbers: 357 W average, 62 kg, a 7.5 kg bike, high end components, 25-28 mm tubeless. Their sheet calculates a mechanical loss of 0.012, a rolling resistance of 0.00351 and a climbing CdA of 0.3442, and returns14:40.

With those same numbers and the patched surface the climb actually has, this calculator gives 14:42: two seconds on the slow side. Set to smooth asphalt, which is what their tyre coefficient assumes, it gives 14:31. The plan sits between the two, which is exactly where it should be.

The drag coefficient used here — 1.09 over the estimated frontal area — comes from matching that 0.3442 CdA; at 1.0, which is what was here before, drag came out 9 % low. And feeding their three exact constants into our equation returns 14:32, so the physics is the same: what changes is the inputs.

Why it does not ask for your sex

Because nothing demonstrated would change in this calculation. What decides the time is mass, power, frontal area and rolling resistance, and the area is estimated from your height and weight, which already carry the size difference. The frontal area regression was built on male cyclists, so for women it may overestimate drag slightly; inventing a coefficient by sex would not fix that. Where sex does change the calculation — body composition — it is asked for.

Where it stops working

  • The calculated time is the ideal one. It assumes power nailed flat, still air and a clear road, and those three do not happen at once. That is why an expected range appears above: power that swings by 10 % costs half a point, a light 10 km/h wind costs another point and a half even blowing half in your favour, and on top goes whatever traffic you pick. The splits table shows the other side: what you gain by placing the watts well.
  • Traffic is declared, not calculated. With a clear road the range sits almost on the ideal time; with buses stopping and slow trucks it runs from 3 to 7 %, which on this climb is one to two minutes. It is a named assumption, not a measurement: nobody has timed how many seconds each overtake costs on the La Calera road. Nor does it count the opposite, which also happens: sitting behind a vehicle for a while lowers drag, but that is not something you plan.
  • There is no wind and no weather. The model assumes still air and a typical morning on the plateau. Putting real wind in means knowing where it blows from and where the road points at each moment: Patios starts north-east, straightens to the north around kilometre 1.5 and ends south-east, so the same wind is a tailwind low down and a headwind higher up. That, with the temperature and humidity of the day, is what gets modelled in the Race Plan, not in a free calculator.
  • The power here is pedal power. It is what your power meter reads, whether it sits at the crank, the pedal or the hub — the last one already discounts part of the loss. What the chain keeps comes from the component level you pick.
  • Performance at altitude is individual. Two cyclists with the same threshold at sea level do not lose the same at 2,600 m. That is measured, not estimated.
The Alto de Patios climb from Usaquén, in Bogotá

When the formula is no longer enough

This is still air. Your race will not be.

The wind on the day, the temperature and the bearing of each corner do not enter here, and on a climb that turns from north to south-east that is minutes. The Race Plan models the whole course with your power curve, the forecast weather and the real route, and returns the target power section by section to load into your head unit.

See the Race Plan
ONEPERFORMANCE FINDER
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