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Vector projection

The vector projection (also known as the vector componentorvector resolution) of a vector a on (or onto) a nonzero vector b is the orthogonal projectionofa onto a straight line parallel to b. The projection of a onto b is often written as ${\displaystyle \operatorname {proj} _{\mathbf {b} }\mathbf {a} }$ora_∥b.

The vector component or vector resolute of a perpendiculartob, sometimes also called the vector rejectionofa from b (denoted ${\displaystyle \operatorname {oproj} _{\mathbf {b} }\mathbf {a} }$ora_⊥b),^[1] is the orthogonal projection of a onto the plane (or, in general, hyperplane) that is orthogonaltob. Since both ${\displaystyle \operatorname {proj} _{\mathbf {b} }\mathbf {a} }$ and ${\displaystyle \operatorname {oproj} _{\mathbf {b} }\mathbf {a} }$ are vectors, and their sum is equal to a, the rejection of a from b is given by: $${\displaystyle \operatorname {oproj} _{\mathbf {b} }\mathbf {a} =\mathbf {a} -\operatorname {proj} _{\mathbf {b} }\mathbf {a} .}$$

To simplify notation, this article defines ${\displaystyle \mathbf {a} _{1}:=\operatorname {proj} _{\mathbf {b} }\mathbf {a} }$ and ${\displaystyle \mathbf {a} _{2}:=\operatorname {oproj} _{\mathbf {b} }\mathbf {a} .}$ Thus, the vector ${\displaystyle \mathbf {a} _{1}}$ is parallel to ${\displaystyle \mathbf {b} ,}$ the vector ${\displaystyle \mathbf {a} _{2}}$ is orthogonal to ${\displaystyle \mathbf {b} ,}$ and ${\displaystyle \mathbf {a} =\mathbf {a} _{1}+\mathbf {a} _{2}.}$

The projection of a onto b can be decomposed into a direction and a scalar magnitude by writing it as ${\displaystyle \mathbf {a} _{1}=a_{1}\mathbf {\hat {b}} }$ where ${\displaystyle a_{1}}$ is a scalar, called the scalar projectionofa onto b, and b̂ is the unit vector in the direction of b. The scalar projection is defined as^[2] $${\displaystyle a_{1}=\left\|\mathbf {a} \right\|\cos \theta =\mathbf {a} \cdot \mathbf {\hat {b}} }$$ where the operator ⋅ denotes a dot product, ‖a‖ is the lengthofa, and θ is the angle between a and b. The scalar projection is equal in absolute value to the length of the vector projection, with a minus sign if the direction of the projection is opposite to the direction of b, that is, if the angle between the vectors is more than 90 degrees.

The vector projection can be calculated using the dot product of ${\displaystyle \mathbf {a} }$ and ${\displaystyle \mathbf {b} }$ as: $${\displaystyle \operatorname {proj} _{\mathbf {b} }\mathbf {a} =\left(\mathbf {a} \cdot \mathbf {\hat {b}} \right)\mathbf {\hat {b}} ={\frac {\mathbf {a} \cdot \mathbf {b} }{\left\|\mathbf {b} \right\|}}{\frac {\mathbf {b} }{\left\|\mathbf {b} \right\|}}={\frac {\mathbf {a} \cdot \mathbf {b} }{\left\|\mathbf {b} \right\|^{2}}}{\mathbf {b} }={\frac {\mathbf {a} \cdot \mathbf {b} }{\mathbf {b} \cdot \mathbf {b} }}{\mathbf {b} }~.}$$

This article uses the convention that vectors are denoted in a bold font (e.g. a₁), and scalars are written in normal font (e.g. a₁).

The dot product of vectors a and b is written as ${\displaystyle \mathbf {a} \cdot \mathbf {b} }$, the norm of a is written ‖a‖, the angle between a and b is denoted θ.

The scalar projection of aonb is a scalar equal to $${\displaystyle a_{1}=\left\|\mathbf {a} \right\|\cos \theta ,}$$ where θ is the angle between a and b.

A scalar projection can be used as a scale factor to compute the corresponding vector projection.

The vector projection of aonb is a vector whose magnitude is the scalar projection of aonb with the same direction as b. Namely, it is defined as $${\displaystyle \mathbf {a} _{1}=a_{1}\mathbf {\hat {b}} =(\left\|\mathbf {a} \right\|\cos \theta )\mathbf {\hat {b}} }$$ where ${\displaystyle a_{1}}$ is the corresponding scalar projection, as defined above, and ${\displaystyle \mathbf {\hat {b}} }$ is the unit vector with the same direction as b: $${\displaystyle \mathbf {\hat {b}} ={\frac {\mathbf {b} }{\left\|\mathbf {b} \right\|}}}$$

By definition, the vector rejection of aonb is: $${\displaystyle \mathbf {a} _{2}=\mathbf {a} -\mathbf {a} _{1}}$$

Hence, $${\displaystyle \mathbf {a} _{2}=\mathbf {a} -\left(\left\|\mathbf {a} \right\|\cos \theta \right)\mathbf {\hat {b}} }$$

When θ is not known, the cosine of θ can be computed in terms of a and b, by the following property of the dot product a ⋅ b $${\displaystyle \mathbf {a} \cdot \mathbf {b} =\left\|\mathbf {a} \right\|\left\|\mathbf {b} \right\|\cos \theta }$$

By the above-mentioned property of the dot product, the definition of the scalar projection becomes:^[2] $${\displaystyle a_{1}=\left\|\mathbf {a} \right\|\cos \theta ={\frac {\mathbf {a} \cdot \mathbf {b} }{\left\|\mathbf {b} \right\|}}.}$$

In two dimensions, this becomes $${\displaystyle a_{1}={\frac {\mathbf {a} _{x}\mathbf {b} _{x}+\mathbf {a} _{y}\mathbf {b} _{y}}{\left\|\mathbf {b} \right\|}}.}$$

Similarly, the definition of the vector projection of a onto b becomes:^[2] $${\displaystyle \mathbf {a} _{1}=a_{1}\mathbf {\hat {b}} ={\frac {\mathbf {a} \cdot \mathbf {b} }{\left\|\mathbf {b} \right\|}}{\frac {\mathbf {b} }{\left\|\mathbf {b} \right\|}},}$$ which is equivalent to either $${\displaystyle \mathbf {a} _{1}=\left(\mathbf {a} \cdot \mathbf {\hat {b}} \right)\mathbf {\hat {b}} ,}$$or^[3] $${\displaystyle \mathbf {a} _{1}={\frac {\mathbf {a} \cdot \mathbf {b} }{\left\|\mathbf {b} \right\|^{2}}}{\mathbf {b} }={\frac {\mathbf {a} \cdot \mathbf {b} }{\mathbf {b} \cdot \mathbf {b} }}{\mathbf {b} }~.}$$

In two dimensions, the scalar rejection is equivalent to the projection of a onto ${\displaystyle \mathbf {b} ^{\perp }={\begin{pmatrix}-\mathbf {b} _{y}&\mathbf {b} _{x}\end{pmatrix}}}$, which is ${\displaystyle \mathbf {b} ={\begin{pmatrix}\mathbf {b} _{x}&\mathbf {b} _{y}\end{pmatrix}}}$ rotated 90° to the left. Hence, $${\displaystyle a_{2}=\left\|\mathbf {a} \right\|\sin \theta ={\frac {\mathbf {a} \cdot \mathbf {b} ^{\perp }}{\left\|\mathbf {b} \right\|}}={\frac {\mathbf {a} _{y}\mathbf {b} _{x}-\mathbf {a} _{x}\mathbf {b} _{y}}{\left\|\mathbf {b} \right\|}}.}$$

Such a dot product is called the "perp dot product."^[4]

By definition, $${\displaystyle \mathbf {a} _{2}=\mathbf {a} -\mathbf {a} _{1}}$$

Hence, $${\displaystyle \mathbf {a} _{2}=\mathbf {a} -{\frac {\mathbf {a} \cdot \mathbf {b} }{\mathbf {b} \cdot \mathbf {b} }}{\mathbf {b} }.}$$

By using the Scalar rejection using the perp dot product this gives

$${\displaystyle \mathbf {a} _{2}={\frac {\mathbf {a} \cdot \mathbf {b} ^{\perp }}{\mathbf {b} \cdot \mathbf {b} }}\mathbf {b} ^{\perp }}$$

The scalar projection aonb is a scalar which has a negative sign if 90 degrees < θ ≤ 180 degrees. It coincides with the length ‖c‖ of the vector projection if the angle is smaller than 90°. More exactly:

• a₁ = ‖a₁‖if0° ≤ θ ≤ 90°,
• a₁ = −‖a₁‖if90° < θ ≤ 180°.

The vector projection of aonb is a vector a₁ which is either null or parallel to b. More exactly:

• a₁ = 0ifθ = 90°,
• a₁ and b have the same direction if 0° ≤ θ < 90°,
• a₁ and b have opposite directions if 90° < θ ≤ 180°.

The vector rejection of aonb is a vector a₂ which is either null or orthogonal to b. More exactly:

• a₂ = 0ifθ = 0°orθ = 180°,
• a₂ is orthogonal to bif0 < θ < 180°,

The orthogonal projection can be represented by a projection matrix. To project a vector onto the unit vector a = (a_x, a_y, a_z), it would need to be multiplied with this projection matrix: $${\displaystyle P_{\mathbf {a} }=\mathbf {a} \mathbf {a} ^{\textsf {T}}={\begin{bmatrix}a_{x}\\a_{y}\\a_{z}\end{bmatrix}}{\begin{bmatrix}a_{x}&a_{y}&a_{z}\end{bmatrix}}={\begin{bmatrix}a_{x}^{2}&a_{x}a_{y}&a_{x}a_{z}\\a_{x}a_{y}&a_{y}^{2}&a_{y}a_{z}\\a_{x}a_{z}&a_{y}a_{z}&a_{z}^{2}\\\end{bmatrix}}}$$

The vector projection is an important operation in the Gram–Schmidt orthonormalizationofvector space bases. It is also used in the separating axis theorem to detect whether two convex shapes intersect.

Since the notions of vector length and angle between vectors can be generalized to any n-dimensional inner product space, this is also true for the notions of orthogonal projection of a vector, projection of a vector onto another, and rejection of a vector from another.

In some cases, the inner product coincides with the dot product. Whenever they don't coincide, the inner product is used instead of the dot product in the formal definitions of projection and rejection. For a three-dimensional inner product space, the notions of projection of a vector onto another and rejection of a vector from another can be generalized to the notions of projection of a vector onto a plane, and rejection of a vector from a plane.^[5] The projection of a vector on a plane is its orthogonal projection on that plane. The rejection of a vector from a plane is its orthogonal projection on a straight line which is orthogonal to that plane. Both are vectors. The first is parallel to the plane, the second is orthogonal.

For a given vector and plane, the sum of projection and rejection is equal to the original vector. Similarly, for inner product spaces with more than three dimensions, the notions of projection onto a vector and rejection from a vector can be generalized to the notions of projection onto a hyperplane, and rejection from a hyperplane. In geometric algebra, they can be further generalized to the notions of projection and rejection of a general multivector onto/from any invertible k-blade.

• Scalar projection
• Vector notation

• Projection of a vector onto a plane