Кольцо под действием двух сосредоточенных моментов смещенных относительно оси

0 < α < θ
M_и = M ⋅ [ 0,3183 ⋅ ( 2 ⋅ cos(α) ⋅ sin(θ) + θ ) - 1 ]
N = M ⋅ 0,6366 ⋅ cos(α) ⋅ sin(θ) ⋅ / r
Q = - M ⋅ 0,6366 ⋅ sin(α) ⋅ sin(θ) ⋅ / r
δ_x = M ⋅ r² ⋅ ( 0,6366 ⋅ θ - sin(θ) ) / (E ⋅ J)

θ < α < π
M_и = M ⋅ [ 0,3183 ⋅ ( 2 ⋅ cos(α) ⋅ sin(θ) + θ ) ]
N = M ⋅ 0,6366 ⋅ cos(α) ⋅ sin(θ) ⋅ / r
Q = - M ⋅ 0,6366 ⋅ sin(α) ⋅ sin(θ) ⋅ / r
δ_y = M ⋅ r² ⋅ ( 0,6366 ⋅ θ + cos(θ) - 1 ) / (E ⋅ J)