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Vector-valued function
A function whose output is a vector (e.g., ⟨x(t), y(t)⟩ or ⟨x(t), y(t), z(t)⟩), often used to represent a particle’s position in 2D/3D over time.
Parameter (t)
An input variable (often time) that drives the component functions in a parametric/vector description of a curve.
Component functions
The scalar functions x(t), y(t), and z(t) that make up a vector-valued function r(t)=⟨x(t), y(t), z(t)⟩.
Position vector
The vector r(t) from the origin to the point (x(t), y(t)) or (x(t), y(t), z(t)) at time/parameter t.
Parametric equations
A way to describe a curve by giving coordinates as functions of a parameter: x=x(t), y=y(t) (and possibly z=z(t)).
Vector form of a parametric curve
Writing parametric equations as a single vector function, e.g., r(t)=⟨x(t), y(t)⟩, representing the same geometric path.
Vertical line test (limitation)
A test for whether a curve is a function y=f(x); many paths (like circles) fail it but can still be represented parametrically.
Componentwise limit (vector-valued)
A vector limit computed by taking limits of each component: lim_{t→a} r(t)=⟨lim x(t), lim y(t)⟩ (and similarly in 3D).
Continuity of a vector-valued function
r(t) is continuous at t=a if each component function is continuous at t=a; any component discontinuity makes r(t) discontinuous.
Differentiating vector-valued functions (componentwise rule)
To differentiate r(t)=⟨x(t), y(t), z(t)⟩, differentiate each component: r′(t)=⟨x′(t), y′(t), z′(t)⟩.
Derivative notation for vector-valued functions
Common ways to write the derivative include r′(t) and d r/dt, meaning the rate of change of the vector with respect to t.
Tangent (direction) vector
For a position function r(t), the derivative r′(t) points in the instantaneous direction of motion along the curve and is tangent to the path.
Parametric slope formula (dy/dx)
For x=x(t), y=y(t), the slope in the xy-plane is dy/dx = (dy/dt)/(dx/dt), provided dx/dt ≠ 0.
Velocity vector
In motion problems, v(t)=r′(t); it gives both the instantaneous speed and direction of motion.
Acceleration vector
a(t)=v′(t)=r″(t); it describes how velocity changes over time (in magnitude and/or direction).
Speed
A scalar equal to the magnitude of velocity: |v(t)| (not the velocity vector itself).
Magnitude of velocity in 2D
If v(t)=⟨x′(t), y′(t)⟩, then |v(t)| = sqrt((x′(t))^2 + (y′(t))^2).
Magnitude of velocity in 3D
If v(t)=⟨x′(t), y′(t), z′(t)⟩, then |v(t)| = sqrt((x′(t))^2 + (y′(t))^2 + (z′(t))^2).
Displacement
The change in position from t=a to t=b: r(b) − r(a) (a vector).
Distance traveled (total path length)
The total length of the path from t=a to t=b: ∫_a^b |v(t)| dt (a scalar).
Recovering position from velocity
If v(t)=r′(t), then r(t) can be found by integrating componentwise: r(t)=∫ v(t) dt, then using an initial condition to find constants.
Initial condition (position)
A given value like r(t0)=⟨x0, y0⟩ used to determine constants of integration when finding r(t) from v(t).
Constants of integration (vector case)
When integrating a vector-valued function, each component may require its own constant (e.g., C1, C2, C3).
Common derivative misconception: |r(t)| vs |v(t)|
|r(t)| is distance from the origin, not speed; speed is |v(t)|, the magnitude of the velocity vector.
Common derivative misconception: d/dt(|r(t)|) vs |r′(t)|
In general, d/dt(|r(t)|) ≠ |r′(t)| because the left is a derivative of a scalar magnitude, while the right is the magnitude of a derivative vector.