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Definite Integral of a Vector-Valued Function
∫abr(t)dt=∫abf(t)dt∫abg(t)dt∫abh(t)dt where r(t)=f(t)g(t)h(t)
Fundamental Theorem of Calculus for Vector Functions
∫abr(t)dt=[R(t)]ab=R(b)−R(a) where R′(t)=r(t)
General Antiderivative of a Vector Function
∫r(t)dt=R(t)+C where R′(t)=r(t) and C=C1C2C3 is a constant vector
Velocity Vector from Acceleration
v(t)=∫a(t)dt+C1 where C1 is determined using the initial condition v(0)=v0
Position Vector from Velocity
r(t)=∫v(t)dt+C2 where C2 is determined using the initial condition r(0)=r0
Projectile Motion Acceleration Vector
a(t)=(0−g) where g=9.8m/s2
Projectile Motion Initial Velocity Vector
v(0)=(v0cos(α)v0sin(α)) where v0 is the launch speed and α is the launch angle
Projectile Motion Velocity Vector
v(t)=(v0cos(α)v0sin(α)−gt)
Projectile Motion Position Vector
r(t)=(x0+(v0cos(α))ty0+(v0sin(α))t−21gt2)
Time to Maximum Height in Projectile Motion
t=gv0sin(α) which occurs when the vertical velocity component satisfies vy(t)=0
Horizontal Range in Projectile Motion
x(t)=(v0cos(α))t evaluated at the time of flight t where the vertical position component satisfies y(t)=0
r(t)
Position vector at time t
v(t)
Velocity vector at time t
a(t)
Acceleration vector at time t
R(t)
Antiderivative vector of r(t)
C
Constant vector of integration
g
Acceleration due to gravity (9.8m/s2)
v0
Initial launch speed (magnitude)
α
Initial launch angle (elevation)
v0
Initial velocity vector at time t=0
r0
Initial position vector at time t=0
t
Elapsed time parameter
x0
Initial horizontal position at time t=0
y0
Initial vertical position at time t=0
vy(t)
Vertical velocity component at time t