So I have been trying to understand the intuitive proof of change of variables in double integrals.
Equations $$ x=x(u, v) \ \mathrm{and} \ y=y(u,v) $$ define a mapping from uv-Cartesian plane to points in xy-plane. The mapping is one-to-one.
The differential area element $$ dA = dx dy$$ is bounded in xy-plane by $$ u, \ u+du,\ v, \ \mathrm{and} \ v+dv.$$ Now the question is, what is dA in uv-plane?
In most intuitive proofs it is said that since du and dv are small and the area element is bounded by smooth curves, the area element is approximately a parallelogram and therefore its are is $$ dA = \left|\vec{AC} \times \vec{AB} \right|=\dots= \left|\frac{\partial(x, y)}{\partial(u, v)} \right| du dv,$$ where $$ \vec{AB}=\frac{\partial x}{\partial u}du\hat{i}+\frac{\partial y}{\partial u}du\hat{j} \ \mathrm{and} \ \vec{AC}=\frac{\partial x}{\partial v}dv\hat{i}+\frac{\partial y}{\partial v}dv\hat{j}.$$
But if we approximate the area element as a parallelogram, shouldn't it be $$ \left \Vert \vec{AB} \right \Vert = du \ \mathrm{and} \ \left \Vert \vec{AC} \right \Vert = dv$$ and therefore we would have a different result for dA?
Edit: So my question really is, are $$ du=\left \Vert \frac{\partial x}{\partial u}du\hat{i}+\frac{\partial y}{\partial u}du\hat{j} \right \Vert \ \mathrm{and} \ dv=\left \Vert \frac{\partial x}{\partial v}dv\hat{i}+\frac{\partial y}{\partial v}dv\hat{j} \right \Vert ?$$
