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Tangential and normal components
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In , given a vector at a point on a , that vector can be decomposed uniquely as a sum of two vectors, one to the curve, called the tangential component of the vector, and another one to the curve, called the normal component of the vector. Similarly, a vector at a point on a surface can be broken down the same way.

More generally, given a N of a M, and a vector in the to M at a point of N, it can be decomposed into the component tangent to N and the component normal to N.


Formal definition

Surface
More formally, let S be a surface, and x be a point on the surface. Let \mathbf{v} be a vector at Then one can write uniquely \mathbf{v} as a sum \mathbf{v} = \mathbf{v}_\parallel + \mathbf{v}_\perp where the first vector in the sum is the tangential component and the second one is the normal component. It follows immediately that these two vectors are perpendicular to each other.

To calculate the tangential and normal components, consider a to the surface, that is, a \hat\mathbf{n} perpendicular to S at Then, \mathbf{v}_\perp = \left(\mathbf{v} \cdot \hat\mathbf{n}\right) \hat\mathbf{n} and thus \mathbf{v}_\parallel = \mathbf{v} - \mathbf{v}_\perp where "\cdot" denotes the . Another formula for the tangential component is \mathbf{v}_\parallel = -\hat\mathbf{n} \times (\hat\mathbf{n}\times\mathbf{v}),

where "\times" denotes the .

These formulas do not depend on the particular unit normal \hat\mathbf{n} used (there exist two unit normals to any surface at a given point, pointing in opposite directions, so one of the unit normals is the negative of the other one).


Submanifold
More generally, given a N of a M and a point p \in N, we get a short exact sequence involving the : T_p N \to T_p M \to T_p M / T_p N The quotient space T_p M / T_p N is a generalized space of normal vectors.

If M is a Riemannian manifold, the above sequence splits, and the tangent space of M at p decomposes as a direct sum of the component tangent to N and the component normal to N: T_p M = T_p N \oplus N_p N := (T_p N)^\perp Thus every v \in T_p M splits as where v_\parallel \in T_p N and v_\perp \in N_p N := (T_p N)^\perp.


Computations
Suppose N is given by non-degenerate equations.

If N is given explicitly, via parametric equations (such as a ), then the derivative gives a spanning set for the tangent bundle (it is a basis if and only if the parametrization is an immersion).

If N is given (as in the above description of a surface, (or more generally as) a ) as a or intersection of for g_i, then the gradients of g_i span the normal space.

In both cases, we can again compute using the ; the cross product is special to 3 dimensions however.


Applications
  • Lagrange multipliers: constrained critical points are where the tangential component of the vanish.
  • Frenet–Serret formulas

  • (1979). 9780486638348, New York: Dover Publications.

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