Given the ODE
we sketch the corresponding surface
On each isocline of height \( C \),
we draw vectors whose slope is \( C \).
For \( C = -8 \): on the curve \( (1-xy)^3 = -8 \) we get \( xy = 3 \), and we draw on the curve vectors with direction \( \theta = \arctan(-8) \approx -83^\circ \).
For \( C = -1 \): on the curve \( (1-xy)^3 = -1 \) we get \( xy = 2 \), and we draw on the curve vectors with direction \( \theta = \arctan(-1) = -45^\circ \).
For \( C = 0 \): on the curve \( (1-xy)^3 = 0 \) we get \( xy = 1 \), and we draw on the curve vectors with direction \( \theta = \arctan(0) = 0^\circ \).
For \( C = 1 \): on the curve \( (1-xy)^3 = 1 \) we get \( xy = 0 \), and the field vector makes the angle \( \theta = \arctan(1) = 45^\circ \).
Continuing this way we obtain the dense direction field. Note that the vectors of the same isocline all point in the same direction — that direction is \( \arctan C \), where \( C \) is the height of the isocline on the surface \( f(x,y) = (1-xy)^3 \).
The solutions of the equation must be tangent to the dense direction field. The panel shows five solutions of the equation for the initial conditions: