Vector-valued functions are powerful tools for describing motion in 3D space. They use a single parameter to define a point's position, allowing us to represent complex curves and trajectories with ease.
These functions are crucial for understanding space curves, helices, and parametric equations . They form the foundation for analyzing motion, calculating limits, and exploring the geometric properties of curves in multivariable calculus.
Vector-Valued Functions
Top images from around the web for Component and unit-vector forms Vectors in Three Dimensions · Calculus View original
Is this image relevant?
Vectors and the Geometry of Space | Boundless Calculus View original
Is this image relevant?
Vector Functions | Boundless Calculus View original
Is this image relevant?
Vectors in Three Dimensions · Calculus View original
Is this image relevant?
Vectors and the Geometry of Space | Boundless Calculus View original
Is this image relevant?
1 of 3
Top images from around the web for Component and unit-vector forms Vectors in Three Dimensions · Calculus View original
Is this image relevant?
Vectors and the Geometry of Space | Boundless Calculus View original
Is this image relevant?
Vector Functions | Boundless Calculus View original
Is this image relevant?
Vectors in Three Dimensions · Calculus View original
Is this image relevant?
Vectors and the Geometry of Space | Boundless Calculus View original
Is this image relevant?
1 of 3
Represents a function that maps a scalar parameter t t t to a vector in 3D space ⟨ f ( t ) , g ( t ) , h ( t ) ⟩ \langle f(t), g(t), h(t) \rangle ⟨ f ( t ) , g ( t ) , h ( t )⟩
f ( t ) f(t) f ( t ) determines the x x x -coordinate based on the value of t t t (time or other parameter)
g ( t ) g(t) g ( t ) determines the y y y -coordinate based on t t t
h ( t ) h(t) h ( t ) determines the z z z -coordinate based on t t t
Component form expresses the vector using ordered triples r ⃗ ( t ) = ⟨ f ( t ) , g ( t ) , h ( t ) ⟩ \vec{r}(t) = \langle f(t), g(t), h(t) \rangle r ( t ) = ⟨ f ( t ) , g ( t ) , h ( t )⟩
Unit-vector form expresses the vector using standard unit vectors r ⃗ ( t ) = f ( t ) i ^ + g ( t ) j ^ + h ( t ) k ^ \vec{r}(t) = f(t)\hat{i} + g(t)\hat{j} + h(t)\hat{k} r ( t ) = f ( t ) i ^ + g ( t ) j ^ + h ( t ) k ^
i ^ \hat{i} i ^ points along the positive x x x -axis ( 1 , 0 , 0 ) (1, 0, 0) ( 1 , 0 , 0 )
j ^ \hat{j} j ^ points along the positive y y y -axis ( 0 , 1 , 0 ) (0, 1, 0) ( 0 , 1 , 0 )
k ^ \hat{k} k ^ points along the positive z z z -axis ( 0 , 0 , 1 ) (0, 0, 1) ( 0 , 0 , 1 )
Parametric equations of space curves
Defines the position of a point on a 3D curve using a parameter t t t
Space curve represented by three equations x = f ( t ) x = f(t) x = f ( t ) , y = g ( t ) y = g(t) y = g ( t ) , z = h ( t ) z = h(t) z = h ( t )
Gives the x x x , y y y , and z z z coordinates as functions of t t t
As t t t varies, the point ( f ( t ) , g ( t ) , h ( t ) ) (f(t), g(t), h(t)) ( f ( t ) , g ( t ) , h ( t )) traces out the curve in 3D space
Parameter t t t often represents time or a position along the curve
Allows representing complex curves not easily expressed using a single equation
Knots, spirals, intersection curves between surfaces
Arc length of a space curve can be calculated using these parametric equations
Helices: shape and equation
3D curve that winds around a central axis at a constant rate
Resembles a spiral staircase or coiled spring
Circular helix with radius a a a , height b b b , centered along z z z -axis has equations:
x = a cos ( t ) x = a\cos(t) x = a cos ( t )
y = a sin ( t ) y = a\sin(t) y = a sin ( t )
z = b t z = bt z = b t
Pitch is the distance between two consecutive turns measured along the helix axis
Equal to 2 π b 2\pi b 2 πb , where b b b is the height parameter
Determines how tightly the helix is wound
Limits of Vector-Valued Functions
Limits of vector-valued functions
Limit of r ⃗ ( t ) \vec{r}(t) r ( t ) as t t t approaches a a a is lim t → a r ⃗ ( t ) \lim_{t \to a} \vec{r}(t) lim t → a r ( t )
Evaluate limit of each component function separately
lim t → a r ⃗ ( t ) = ⟨ lim t → a f ( t ) , lim t → a g ( t ) , lim t → a h ( t ) ⟩ \lim_{t \to a} \vec{r}(t) = \langle \lim_{t \to a} f(t), \lim_{t \to a} g(t), \lim_{t \to a} h(t) \rangle lim t → a r ( t ) = ⟨ lim t → a f ( t ) , lim t → a g ( t ) , lim t → a h ( t )⟩
Limit exists if all component limits exist, equals vector of component limits
Limit doesn't exist if any component limit doesn't exist
Continuous at a a a if lim t → a r ⃗ ( t ) = r ⃗ ( a ) \lim_{t \to a} \vec{r}(t) = \vec{r}(a) lim t → a r ( t ) = r ( a )
Value of the function at a a a equals the limit as t t t approaches a a a
Frenet-Serret Frame and Curve Properties
Tangent, Normal, and Binormal Vectors
Tangent vector is the derivative of the position vector, indicating the direction of motion along the curve
Normal vector is perpendicular to the tangent vector and points towards the center of curvature
Binormal vector is perpendicular to both tangent and normal vectors, forming a right-handed coordinate system
Curvature and Torsion
Curvature measures how sharply a curve bends at each point
Torsion quantifies how much a curve twists out of a plane, with zero torsion indicating a planar curve