Drilling guides › Directional survey calculations: minimum curvature step by step

Directional survey calculations: minimum curvature step by step

By the DrillPro team · Last reviewed 9 November 2026

A directional survey measures where the hole is pointing at a given depth along the hole. From a series of those measurements we calculate where the hole actually is: how deep vertically, and how far north and east of the surface location. Those positions decide whether the well hits its target, whether it stays clear of nearby wells, and what the true vertical depth is for every pressure calculation. Getting them right matters well beyond the directional driller's office.

The terms

TermMeaning
Measured depth (MD)Length along the hole from the depth reference (usually the rotary table or drill floor).
Inclination (I)Angle of the hole from vertical: 0° is vertical, 90° is horizontal.
Azimuth (A)Direction of the hole in the horizontal plane, measured clockwise from north, 0° to 360°. State which north: true, grid or magnetic.
True vertical depth (TVD)Vertical distance below the reference. Hydrostatic and formation pressures use TVD.
Northing, eastingHorizontal displacement north (negative = south) and east (negative = west) of the well's surface location.
Dogleg (DL)Total change in hole direction between two stations, combining inclination and azimuth change.
Dogleg severity (DLS)Dogleg per 100 ft of MD (or per 30 m in metric).

A survey tool only gives MD, inclination and azimuth. Everything else is calculated, and the result depends on how we assume the hole bends between stations.

The dogleg

The dogleg is the angle between the two direction vectors of the hole at the upper and lower stations. It is found from:

cos DL = cos(I₂ − I₁) − sin I₁ × sin I₂ × (1 − cos(A₂ − A₁)) DLS (°/100 ft) = DL (°) × 100 ÷ ΔMD (ft)

The second term shows something that surprises many people: a change in azimuth counts for little in a near-vertical hole, because sin I is small, but counts fully in a horizontal one. A 6° turn at 10° inclination is a mild dogleg; the same turn at 60° is a severe one.

Dogleg severity matters because pipe running through a dogleg is bent, and under tension it is pressed against the wall. High DLS raises torque and drag, wears casing, causes key seats, and gives fatigue in rotating drill pipe. Casing and completion design often limit the DLS that can be accepted in parts of the well.

Minimum curvature method

The minimum curvature method assumes the hole between two stations is the smoothest possible curve: a circular arc lying in one plane, tangent to the measured direction at each station. It is the industry standard for final well positions. The steps are:

  1. Find the dogleg DL from the formula above, in radians for the next step.
  2. Find the ratio factor RF, which corrects the straight-line averages for the curvature of the arc.
  3. Calculate the changes in north, east and vertical depth, and add them to the upper station's position.
RF = (2 ÷ DL) × tan(DL ÷ 2) (DL in radians; RF = 1 when DL = 0) ΔN = ΔMD ÷ 2 × (sin I₁ cos A₁ + sin I₂ cos A₂) × RF ΔE = ΔMD ÷ 2 × (sin I₁ sin A₁ + sin I₂ sin A₂) × RF ΔTVD = ΔMD ÷ 2 × (cos I₁ + cos I₂) × RF

For normal survey intervals, RF is only a little more than 1. Its main purpose is to make the method consistent for any dogleg. A common mistake is to calculate DL in degrees and then use it in the RF formula, which needs radians. If DL is zero (a perfectly straight section), the formula would divide by zero; set RF to 1.

Worked example 1: two stations by minimum curvature

Upper station: MD 5,000 ft, I 10°, A 40°. Position TVD 4,962.4 ft, N 210.3 ft, E 168.7 ft. Lower station: MD 5,100 ft, I 14°, A 48°. ΔMD = 100 ft.

Step 1: dogleg cos(I₂ − I₁) = cos 4° = 0.997564 sin 10° × sin 14° × (1 − cos 8°) = 0.000409 cos DL = 0.997564 − 0.000409 = 0.997155 DL = 4.323° = 0.075447 rad DLS = 4.32°/100 ft (4.25°/30 m) Step 2: ratio factor RF = (2 ÷ 0.075447) × tan(0.037724) = 1.00047 Step 3: displacements sin I₁ cos A₁ = 0.13302 sin I₂ cos A₂ = 0.16188 sin I₁ sin A₁ = 0.11162 sin I₂ sin A₂ = 0.17978 cos I₁ = 0.98481 cos I₂ = 0.97030 ΔN = 50 × (0.13302 + 0.16188) × 1.00047 = 14.75 ft ΔE = 50 × (0.11162 + 0.17978) × 1.00047 = 14.58 ft ΔTVD = 50 × (0.98481 + 0.97030) × 1.00047 = 97.80 ft Lower station: TVD 5,060.2 ft, N 225.1 ft, E 183.3 ft

The hole went 100 ft along its length but only 97.8 ft deeper, and moved about 20.7 ft sideways in that interval.

Simpler methods for comparison

Older or quick methods treat the interval as a straight line.

Method (same two stations)ΔN (ft)ΔE (ft)ΔTVD (ft)
Minimum curvature14.7514.5897.80
Average angle (I 12°, A 44°)14.9614.4497.81
Tangential (I 14°, A 48°)16.1917.9897.03

Over one interval the tangential method is already 3.4 ft off to the east. Over a few hundred stations, that kind of bias can put a well far from where it really is.

Worked example 2: an azimuth change at high angle

Two stations 90 ft apart, both at 60° inclination. The azimuth turns from 120° to 126°.

cos DL = cos 0° − sin 60° × sin 60° × (1 − cos 6°) = 1 − 0.75 × 0.005478 = 0.995891 DL = 5.196° DLS = 5.196 × 100 ÷ 90 ≈ 5.77°/100 ft Same turn at 10° inclination: DLS ≈ 1.16°/100 ft

Minimum curvature gives ΔN = −42.42 ft, ΔE = +65.32 ft and ΔTVD = 45.03 ft for this interval. The negative northing means the hole is heading south of east, as an azimuth between 90° and 180° should. A turn of only 6° is close to 6°/100 ft of dogleg severity here, which could already exceed a casing wear or completion limit.

Closure and vertical section

Two more numbers appear on every survey report. The closure is the straight-line horizontal distance from the surface location to the station, √(N² + E²), with its direction. The vertical section is the horizontal displacement projected onto a chosen plane, usually the direction from the surface location to the target: VS = closure × cos(target azimuth − closure azimuth). The directional driller steers to keep the well on the planned vertical section and TVD. For the lower station in example 1, the closure is √(225.1² + 183.3²) ≈ 290.3 ft towards 39.2°; with a target direction of 45°, the vertical section is about 288.8 ft.

Where survey errors come from

The calculation is exact for its assumptions, but the inputs are not. Magnetic tools are disturbed by nearby casing, steel in the BHA and the earth's changing field. Depth is measured on pipe that stretches and is corrected only roughly. Inclination sensors drift. Each survey therefore has an uncertainty, which grows with depth and is shown as an ellipse around the calculated position. That is why anti-collision work uses the uncertainty ellipses, and not only the calculated centre line, when deciding whether two wells are too close.

Metric notes

The formulas are the same with MD in metres; the displacements come out in metres. DLS is usually quoted per 30 m. Since 30 m is 98.43 ft, °/30 m = °/100 ft × 0.984.

Good practice

Run your survey calculations in DrillPro

DrillPro does these sums for you on Android, the web and desktop, and exports the result to PDF or Excel.