Built by a geologist
Geothermal Gradient and Formation Temperature Calculator
Geothermal gradient describes temperature change per unit increase in depth. For a reference temperature T1 at positive-down depth z1 and a constant interval gradient G, a simple linear estimate is T2 = T1 + G times the difference between target depth z2 and reference depth z1. Rearranging solves reference temperature as T1 = T2 minus G times the depth interval, average gradient as G = the temperature difference divided by the depth difference, or target depth as z2 = z1 + the temperature difference divided by G. GeoMiner solves all four directions. Temperature inputs and outputs support degrees Celsius and Fahrenheit. Depth supports metres, feet, kilometres, and miles. Gradient supports degrees Celsius per kilometre, degrees Celsius per 100 metres, and degrees Fahrenheit per 100 feet. Unit conversion normalizes temperatures to Celsius, depths to metres, and gradient to degrees Celsius per kilometre before calculation. Both depths must use one declared vertical datum. In a deviated borehole, measured hole depth is longer than true vertical depth and cannot be substituted into a vertical geothermal gradient without justified geometry. Reference temperature and reference depth must describe the same physical point and condition. Land-surface air temperature, mean annual ground temperature, shallow groundwater temperature, seafloor or mudline temperature, and a temperature logged within a borehole are not interchangeable. Solving a gradient from two points returns one straight-line interval average. It does not prove that the local derivative is constant between, above, or below those points. Temperature gradients can change with rock thermal conductivity, lithology, layering, heat flow, radioactive heat production, sedimentation and erosion, topography, climate history, faults, intrusions, groundwater and hydrothermal advection, borehole flow, and measurement disturbance. Heat flow is not temperature gradient under another name. Conductive heat flow also requires representative thermal conductivity and a stated sign convention, while advective or transient conditions require a broader thermal model. Bottom-hole temperatures measured soon after drilling or fluid circulation commonly do not represent equilibrium formation temperatures. Correction validity depends on measurement method, shut-in and circulation history, basin calibration, data quality, and thermal