A close look at one specific problem — minimize \((x-2)^2+(y-2)^2\) subject to \(x+y-2<0\) — that reveals a fact with nothing to do with quadratics at all.
The dual function is the lowest point of a whole family of straight lines — one line per point in the primal domain. However you tilt and place a bunch of straight lines, the shape traced by their lowest points is always a dome, never a saddle. That's the entire reason. The fact that \(f\) is a quadratic bowl never enters into it.
\(f(x,y)=(x-2)^2+(y-2)^2\) is a paraboloid bowl with its bottom sitting at \((2,2)\). The constraint \(x+y-2<0\) fences off half the plane — everything on one side of the diagonal line \(x+y=2\) is off-limits.
Notice immediately: the bowl's true bottom, \((2,2)\), gives \(x+y-2=2\), which is on the wrong side of the fence. So the constrained problem is genuinely constrained — the fence is doing real work, not just standing there decoratively.
Pick any single spot \((x,y)\) and hold it fixed. The Lagrangian charges a price \(\lambda\) for standing on the wrong side of the fence:
\[ L(x,y,\lambda) = f(x,y) + \lambda\,(x+y-2) \]
For a fixed point, this is embarrassingly simple: it's just a straight line in \(\lambda\). The intercept is \(f(x,y)\) — what you pay at zero price. The slope is \(x+y-2\) — how far over the fence you are.
The dual function doesn't fix one point — it asks, for every price \(\lambda\), which point is cheapest right now?
\[ g(\lambda) = \min_{x,y} L(x,y,\lambda) \]
That means \(g(\lambda)\) is the pointwise minimum, over every point in the plane, of a straight line. Add lines below, one per point. Watch what their lower boundary does as more arrive.
For this particular \(f\) we can do the inner minimization with calculus. Setting \(\partial L/\partial x = \partial L/\partial y = 0\):
\[ x^*(\lambda) = y^*(\lambda) = 2 - \tfrac{\lambda}{2} \]
Substituting back gives a closed form for the dome we built numerically above:
\[ g(\lambda) = 2\lambda - \tfrac{\lambda^2}{2}, \qquad g''(\lambda) = -1 \]
Drag \(\lambda\) below. Watch the optimal point slide along the diagonal in the bowl, and watch its line rotate until it exactly grazes the envelope at that \(\lambda\) — because that's the definition of the envelope: the one line, among infinitely many, that happens to be lowest right there.
Restate the kernel with the specifics now filled in: \(g(\lambda)=\min_{x,y}L(x,y,\lambda)\) is a minimum, taken over \((x,y)\), of a function that is affine in \(\lambda\) for every fixed \((x,y)\). A pointwise minimum of affine functions is concave — full stop, no assumptions on \(f\) required. Step 3 showed it by brute force (pile up lines, watch the dome emerge); Step 4 confirmed it in closed form for this specific quadratic.
What quadratics do buy you, separately, is strong duality — the dome's peak, \(g(2)=2\), exactly matches the primal optimum \(f(1,1)=2\). That's Slater's condition doing its job (a convex feasible region with an interior point), and it's a second, independent fact. Swap \(f\) for something nonconvex and \(g(\lambda)\) is still, provably, a dome — you'd just lose the guarantee that its peak reaches the true primal answer.
The dual is concave because it's a minimum over a family of straight lines — and no family of straight lines can ever have a lower envelope shaped like anything but a dome.