How to solve the quadratic form I am a physicist and I have a problem solving this
\begin{equation}
Q(x)=\frac{1}{2}(x,Ax)+(b,x)+c
\end{equation}
In a book it says that:
"The minimum of Q lies at $\bar{x}=-A^{-1}b$ and
\begin{equation}
Q(x)=Q(\bar{x})+\frac{1}{2}((x-\bar{x}),A(x-\bar{x}))
\end{equation}
How do I go to this? What how much is $Q(\bar{x})$?

The stated properties are analogues of those of the single-variable function $q:x\mapsto\frac12ax^2+bx+c$, for which the minimum occurs at $\bar x=-\frac ba$ (when $a\gt0$) and $q(x)=q(\bar x)+\frac12a(x-\bar x)^2$. It can be derived in a completely analogous fashion to the single-variable case.
Assuming that $A=A^T$, we have $\nabla Q(x)=\frac12(A+A^T)x+b=Ax+b$. The critical points occur where the gradient vanishes, so if $A$ is nonsingular this is at the unique point $\bar x=-A^{-1}b$. Since $Q(\bar x)$ is stated to be a minimum, we also have that $A$ is positive-definite: the graph of $Q$ is an elliptic paraboloid with vertex at $(\bar x; Q(\bar x))$.  
The Hessian of $Q$ is $A$ and higher-order derivatives vanish, so by Taylor’s theorem, $$Q(x)=Q(\bar x)+\langle\nabla Q(\bar x),x-\bar x\rangle+\frac12\langle x-\bar x,A(x-\bar x)\rangle,$$ but $\nabla Q(\bar x)$ vanishes, leaving the desired equation.  
As for the value of $Q(\bar x)$, finding that is a simple matter of substitution: $$\begin{align} Q(\bar x) &= \frac12\langle\bar x,A\bar x\rangle+\langle b,\bar x\rangle+c \\ &= \frac12\langle A^{-1}b,b\rangle-\langle b,A^{-1}b\rangle+c \\ &= c-\frac12\langle b,A^{-1}b\rangle. \end{align}$$ (Here we’ve again used the fact that $A=A^T$.) Compare this to the single-variable case, for which the vertex of the parabola is at $\left(-\frac ba,c-{b^2\over2a}\right)$.
