A cone with vertex at the origin and opening upward, with axis along the positive -axis, is scaled (stretched) along the -axis direction by a factor of 2. The angle between the surface of the unstretched cone and its axis, is . A plane with equation cuts though this stretched cone. The intersection between the plane and the stretched cone is an ellipse. Find the sum of the semi-minor and semi-major axes of this ellipse.
Round your answer to three decimal places.
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Equation of regular cone, with angle θ c between its surface and its axis, is:
r ⋅ k ^ = cos θ c ∣ r ∣
Let r' be the corresponding point on the stretched cone, then
r ′ = S r
where
S = ⎣ ⎡ S x 0 0 0 S y 0 0 0 S z ⎦ ⎤
Thus r = S − 1 r ′
Thus for a stretched cone, its equation is obtained by replacing the vector r with S − 1 r ′ ,
So, we have,
( ( S − 1 r ′ ) . k ) 2 = cos 2 θ c ( S − 1 r ′ ) ⋅ ( S − 1 r ′ )
hence the equation becomes
r T Q r = 0
where
Q = S − 1 ( k k T − cos 2 θ c I ) S − 1
at the final step, I replaced r ′ with r , for notation simplicity.
Now, the equation of the cutting plane in vector form is r = r 0 + V u , where V = [ v 1 , v 2 ] , where v 1 , v 2 are two unit vectors that are orthogonal to each other and to the normal to the plane. u is the coordinate vector with respect to v 1 and v 2 .
Substituting this into the equation of the stretched cone,
( r 0 + V u ) T Q ( r 0 + V u ) = 0
Expanding
u T V T Q V u + 2 r 0 T Q V u = − r 0 T Q r 0
the left hand side can be rewritten as
( u − u 0 ) T V T Q V ( u − u 0 ) − u 0 T V T Q V u 0
where u 0 = − ( V T Q V ) − 1 V T Q r 0
Hence,
( u − u 0 ) T V T Q V ( u − u 0 ) = u 0 T V T Q V u 0 − r 0 T Q r 0
Define A = V T Q V and c = u 0 T V T Q V u 0 − r 0 T Q r 0 , then we have
( u − u 0 ) T A ( u − u 0 ) = c
Dividing both sides by c,
( u − u 0 ) T B ( u − u 0 ) = 1
where B = A / c
Since B is symmetric, we can find a rotation matrix (an orthogonal matrix) R and a diagonal matrix D, such that
R T B R = D
Note that
R = [ cos θ sin θ − sin θ cos θ ]
This suggests the change of variable, u = u 0 + R w , that leads to the simpified expression
w T D w = 1
Thus with respect to the w-coordinate frame, this is an ellipse with semi-major and semi-minor axes equal to the reciprocal of the square roots of the diagonal elements of D.
Note that since u and w are related by a translation and a rotation then these dimensions remain unchanged when moving from the w-coordinates to the u-coordinates.
In particular, since u = u 0 + R w , and since R is a rotation matrix by an angle θ , then with respect to the u-coordinate frame, this is an ellipse centered at u_0, with its axes rotated by the angle θ .
And finally, r = r 0 + V u = r 0 + V ( u 0 + R w ) = r 0 + V u 0 + V R w
Therefore, r describes an ellipse centered at r 0 + V u 0 , having its major and minor axes in the plane spanned by { v 1 , v 2 } , rotated by angle θ from the direction of v 1 and v 2 .
Making the necessary calculations, we obtain a semi-minor axis of m = 2 0 . 7 0 2 7 6 and a semi-major axis of M = 4 4 . 0 2 9 8 4 8 , making the answer M + m = 6 4 . 7 3 3