How to get the limits of rotated ellipse? The box that an ellipse fits is easily calculated if there are no rotation, or if the rotation is ${x*90^o}$ (where x is an integer) is easy.
For a (major radius) and b (minor radius), it is :  
Xmax = a
Ymax = b

or it is :  
Xmax = b
Ymax = a

But how to do it in a general case, when the rotation angle is not a multiple of 90 degrees?
The limits to ellipse are like on the next image:

I am given all ellipse's parameter (as described in wiki) :


*

*ellipses formula:
  $x_{0}=a\cdot \cos (\varphi )$
  $y_{0}=b\cdot \sin (\varphi )$


*

*where: a=major radius, b=minor radius, $\varphi \in  [0,\pi ]$


*rotation formula:
  $x_{1}=x_{0}\cdot \cos (\Theta )-y_{0}\cdot \sin (\Theta )$
  $y_{1}=x_{0}\cdot \sin (\Theta )+y_{0}\cdot \cos (\Theta )$  


*

*where $\Theta$=ellipse's rotation



All parameters (a, b and $\Theta$) are known.
If you like you can also use the canonical form for ellipse: $\frac{x^2}{a^2}+\frac{y^2}{b^2}=1$
 A: You don't need calculus here, just a little geometry.  
Let $c$ be the (positive) $x$-coordinate of the vertical tangent, and let $d$ be the (positive) $y$-coordinate where the rotated ellipse meets the $y$-axis. Apply a vertical shear transformation, of the form $(x,y) \mapsto (x,y+ux)$, to transform the rotated ellipse into an ellipse with horizontal major axis $c$ and vertical minor axis $d$. This transformation is area-preserving, so $\pi cd = \pi ab$. Thus $c = ab/d$.  
To find $d$, take the equation of the rotated ellipse (filched from J.M.'s answer):
$$\frac{(x\cos\theta-y\sin\theta)^2}{a^2}+\frac{(x\sin\theta+y\cos\theta)^2}{b^2}=1$$
and set $x = 0$:
$$\frac{(d\sin\theta)^2}{a^2}+\frac{(d\cos\theta)^2}{b^2}=1$$
Hence
$$\frac{d^2}{a^2b^2}(b^2\sin^2\theta+a^2\cos^2\theta) = 1$$
giving
$$c = \frac{ab}{d} = \sqrt{b^2\sin^2\theta+a^2\cos^2\theta}$$
Similarly, using a horizontal shear transformation, the $y$-coordinate of the horizontal tangent is $\sqrt{a^2\sin^2\theta+b^2\cos^2\theta}$.
A: The previous answerer had the right idea, but the wrong execution. We have, for the rotated ellipse
$$\frac{(x\cos\,\theta-y\sin\,\theta)^2}{a^2}+\frac{(x\sin\,\theta+y\cos\,\theta)^2}{b^2}=1$$
the following expression for the derivative:
$$\frac{\mathrm dy}{\mathrm dx}=-\frac{a^2 x\,\sin^2\theta+y(a-b)(a+b)\sin\,\theta \cos\,\theta+b^2 x\,\cos^2\theta}{a^2 y\,\cos^2\theta+x(a-b)(a+b)\sin\,\theta \cos\,\theta+b^2 y\,\sin^2\theta}$$
We can separate the numerator and denominator of this expression, and equate any of the two to zero, and then solve as a simultaneous equation with the equation of the ellipse. (Zero numerator corresponds to horizontal tangents, and zero denominator corresponds to vertical tangents.)
After much algebra and tears, we find that the required limits are $x=\pm\sqrt{a^2\cos^2\theta+b^2\sin^2\theta}$ and $y=\pm\sqrt{a^2\sin^2\theta+b^2\cos^2\theta}$.
This could also have been done starting from the parametric equations; for that route, one will need to use the Weierstrass substitution so that one has the rational parametrization of the ellipse, and the problem is reduced again to the solution of algebraic equations.

Here is a Mathematica demonstration:
With[{a = Sqrt[2], b = 1, th = Pi/6}, 
 Block[{xa = Sqrt[a^2 Cos[th]^2 + b^2 Sin[th]^2], 
        ya = Sqrt[a^2 Sin[th]^2 + b^2 Cos[th]^2]}, 
       ParametricPlot[
         RotationMatrix[th].{a Cos[u], b Sin[u]}, {u, 0, 2 Pi}, 
         Epilog -> {AbsoluteThickness[4], 
         Line[{{-xa, -ya}, {xa, -ya}, {xa, ya}, {-xa, ya}, {-xa, -ya}}]}
      ]]]


A: Let the equation of the ellipse be $\frac{X^2}{a^2}+\frac{Y^2}{b^2}=1$ in the rotated frame. The equation of tangent at parametric coordinate $\alpha$ becomes after rotation to the original frame $$ x\left(\cos\theta \cos\alpha/a+\sin\theta\sin\alpha/b\right)+y\left(\cos\theta \sin\alpha/a-\sin\theta\cos\alpha/b\right)=1$$
We need the tangents with slope 0 and inf. This gives the required lines as 
$$x=\frac{ab}{a\sin\theta\sin\phi+b\cos\theta\cos\phi}$$ and 
$$y=\frac{ab}{b\sin\theta\sin\phi+a\cos\theta\cos\phi}$$
where $\tan\phi=\frac ab\tan\theta$.
