applications of vectors

Work

Work is the force applied onto an object over a distance.

You can calculate the work done on an object by using the dot product:

Work = = magnitude of a force F⃗ \vec {F} along d⃗ × \vec {d} \ \times magnitude of displacement

 =∣ projd⃗F⃗ ∣×∣ d⃗ ∣ \quad \quad \ = | \ \text {proj}_{ \vec {d} } \vec {F} \ | \times | \ \vec {d} \ |

 =∣ F⃗ ⋅ d⃗ ∣∣ d⃗ ∣×∣ d⃗ ∣ \quad \quad \ = \frac {| \ \vec {F} \ \cdot \ \vec {d} \ |} {| \ \vec {d} \ |} \times | \ \vec {d} \ |

 =∣ F⃗ ⋅ d⃗ ∣ \quad \quad \ = | \ \vec {F} \ \cdot \ \vec {d} \ |


So, the work for a force F⃗ \vec {F} along a distance d⃗ \vec {d} is:

Work=∣ F⃗ ⋅ d⃗ ∣ \text {Work} = | \ \vec {F} \ \cdot \ \vec {d} \ |

Torque

Torque is a vector quantity, denoted as τ⃗ \vec { \tau } , is the measure of force applied about an axis in order to rotate an object.

Torque can be calculated using the cross product of the radius r⃗ \vec {r} from the object, and the force F⃗ \vec {F} applied:

∣ τ⃗ ∣=∣ r⃗×F⃗ ∣=∣ r⃗ ∣∣ F⃗ ∣sin⁡θ | \ \vec {\tau} \ | = | \ \vec {r} \times \vec {F} \ | = | \ \vec {r} \ | | \ \vec {F} \ | \sin \theta

Area of a parallelogram

The area of a parallelogram formed by an upper vector a⃗ \vec {a} and a lower vector b⃗ \vec {b} is given by the magnitude of the cross product of both vectors:

A=∣ a⃗×b⃗ ∣=∣ a⃗ ∣∣ b⃗ ∣sin⁡θ A = | \ \vec {a} \times \vec {b} \ | = | \ \vec {a} \ | | \ \vec {b} \ | \sin \theta

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Volume of a parallelepiped

The volume of a parallelepiped formed by a vector c⃗ \vec {c} and two lower vectors a⃗ \vec {a} and b⃗ \vec {b} is given by the magnitude of the cross product of both vectors:

V=∣ a⃗ ⋅ (b⃗×c⃗) ∣ V = | \ \vec {a}\ \cdot \ (\vec {b} \times \vec {c}) \ |