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Boussinesq stress below circle center

Short answer

Integrating the Boussinesq point load over a circular area gives Δσz = q[1 − 1/(1+(R/z)2)3/2]. For R = 2 m, q = 100 kPa, stresses at z = 1, 2, 4 m are 91.1, 64.6, 28.4 kPa.

Using Boussinesq's equation for point load, determine the increment in vertical stress below the center of a uniformly loaded circle. Assume all necessary conditions.

Assumptions

Uniform pressure qq on a flexible circular area of radius RR on the ground surface; the soil is homogeneous, isotropic and elastic (Boussinesq). The stress is required at depth zz below the centre.

Derivation

Boussinesq's equation for a point load dQdQ at horizontal distance rr:

dσz=3 dQ2πz2[11+(r/z)2]5/2d\sigma_z = \frac{3\,dQ}{2\pi z^2}\left[\frac{1}{1+(r/z)^2}\right]^{5/2}

An elemental ring of radius rr and width drdr carries dQ=q (2πr dr)dQ = q\,(2\pi r\,dr). All points of the ring are at the same distance rr from the axis, so:

Δσz=∫0R3q (2πr dr)2πz2[11+(r/z)2]5/2=3q∫0Rr drz2[1+r2z2]−5/2\Delta\sigma_z = \int_0^R \frac{3q\,(2\pi r\,dr)}{2\pi z^2}\left[\frac{1}{1+(r/z)^2}\right]^{5/2} = 3q\int_0^R \frac{r\,dr}{z^2}\left[1+\frac{r^2}{z^2}\right]^{-5/2}

Let t=1+r2/z2t = 1 + r^2/z^2, so dt=2r dr/z2dt = 2r\,dr/z^2:

Δσz=3q2∫11+R2/z2t−5/2 dt=q[1−1(1+(R/z)2)3/2]\Delta\sigma_z = \frac{3q}{2}\int_1^{1+R^2/z^2} t^{-5/2}\,dt = q\left[1 - \frac{1}{\left(1+(R/z)^2\right)^{3/2}}\right] Δσz=q[1−1(1+(R/z)2)3/2]\boxed{\Delta\sigma_z = q\left[1 - \frac{1}{\left(1+(R/z)^2\right)^{3/2}}\right]}

Example

Take q=100q = 100 kPa and R=2R = 2 m.

zz (m)R/zR/zΔσz\Delta\sigma_z (kPa)
12.091.1
21.064.6
40.528.4

The stress decreases with depth, and is nearly qq close to the surface.

✓ Answer checked by Claude Opus 5.5 (high effort)

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