15.13
Consider a paraboloid surface where r represents the position vector of any point on the surface. Using x and y as parameters, the surface can be described parametrically.
A tangent plane is a flat surface that touches this curved surface at a single unique point. Consequently, the tangent plane contains the tangent vectors to any curved paths along the surface that pass through this point.
The partial derivative rx gives the tangent vector in the x direction, and the partial derivative ry gives the tangent vector in the y direction.
Evaluating these at point A gives the tangent vectors in the x and y directions contained in the tangent plane.
Their cross product gives a normal vector n perpendicular to the tangent plane.
For any point P in the tangent plane, the vector v from A to P lies in the plane and is therefore perpendicular to the plane’s normal vector n.
As a result, the dot product of the vector n and v is zero. Expanding this dot product and simplifying gives the final equation of the tangent plane at point A to the given surface.
A tangent plane provides a linear approximation to a curved surface at a specific point, capturing the local behavior of the surface. It can be understood as the plane that just touches the surface at that point and is defined by the tangent directions of curves lying on the surface. These tangent directions arise naturally when the surface is described parametrically, allowing systematic construction of the plane.
For a surface expressed in parametric form, the position of any point is determined by two parameters. At a fixed point on the surface, varying each parameter independently traces curves along the surface. The partial derivatives with respect to these parameters produce tangent vectors that lie along these curves. One vector corresponds to variation in the first parameter, while the other corresponds to variation in the second parameter. Evaluating these vectors at the point of interest provides two independent directions that span the tangent plane.
The cross product of the two tangent vectors produces a normal vector perpendicular to the surface at the given point. This normal vector is essential for defining the orientation of the tangent plane. Any point lying on the plane can be connected to the point of tangency by a vector that remains entirely within the plane. Because the normal vector is perpendicular to the plane, this connecting vector must be orthogonal to the normal direction.
The defining property of the tangent plane is that any vector within it forms a right angle with the normal vector. This orthogonality condition provides a concise way to characterize the plane. By expressing the relationship between a general point on the plane and the point of tangency, and enforcing perpendicularity to the normal vector, the complete description of the tangent plane is obtained.
Consider a paraboloid surface where r represents the position vector of any point on the surface. Using x and y as parameters, the surface can be described parametrically.
A tangent plane is a flat surface that touches this curved surface at a single unique point. Consequently, the tangent plane contains the tangent vectors to any curved paths along the surface that pass through this point.
The partial derivative rx gives the tangent vector in the x direction, and the partial derivative ry gives the tangent vector in the y direction.
Evaluating these at point A gives the tangent vectors in the x and y directions contained in the tangent plane.
Their cross product gives a normal vector n perpendicular to the tangent plane.
For any point P in the tangent plane, the vector v from A to P lies in the plane and is therefore perpendicular to the plane’s normal vector n.
As a result, the dot product of the vector n and v is zero. Expanding this dot product and simplifying gives the final equation of the tangent plane at point A to the given surface.
From Chapter 15:
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