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average velocity
represented by the equation of vector v avg = vector r - vector r0 / t - t0
thus vector v avg = vector ∆r / ∆t
vector ∆r is the displacement
∆t is the change in time or the time interval
average velocity describes the change in position
velocity is the the vector
parallel to displacement telling how quickly it occurred and the direction
independent of position
average speed
average speed is equal to distance / elapsed time
there is no information about the direction of motion
instantaneous velocity is the
instantaneous rate at which position changes (a more accurate description of motion rather than that of average velocity)
represented by the equation vector v avg = lim ∆t → 0 vector ∆r / ∆t
small ∆t value can be thought of as an instant
instantaneous velocity compares
intermediate positions
the average slope of the position vs. time graph shows the average rate of change of x with time (average velocity)
the slope of the tangent to the position vs. time graph at a specific point and time interval gives the instantaneous velocity
motion with constant velocity
if the vector v (velocity) is constant, the position of the object changes at a constant rate
mathematically, displacement is proportional to elapsed time
represented by the equation x(t) = x0 + vt (rearranged from the average velocity equation v = x - x0 / t - t0, when t0 = 0
velocity describes the
instantaneous direction of motion
acceleration is the
rate at which velocity changes (rate of change of velocity)
average acceleration is represented by the equation vector a avg = vector v - vector v0 / t - t0 = vector ∆v / ∆t
vector ∆v is the change in velocity
∆t is the change in time
average acceleration is always parallel ot the change in velocity (vector ∆v)
acceleration has
different dimensions than velocity and is on a different scale
instantaneous acceleration is a
more accurate description of the change in velocity
represented by the equation vector a = lim ∆t → 0 vector ∆v / ∆t
acceleration vector tells us the rate and direction of velocity change
velocity vector can change in magnitude only, direction only, or both (results in acceleration change)
acceleration may correspond to either an
increase or decrease in speed
if acceleration is in the same direction as velocity, the
speed increases
velocity will have a greater magnitude
either positive or negative acceleration
vector v initial + vector ∆v = vector v final
if acceleration is in the opposite direction as velocity, the
speed decreases
velocity will have a smaller magnitude
either positive or negative acceleration
vector v initial - vector ∆v = vector v final
negative acceleration does not mean
decreasing speed
if the acceleration vector is constant, then
velocity changes at a constant rate
one dimensional
if t0 = 0, then the equation is v(t) = v0 + at (velocity as a function of time)
rearranged from the equation a = v(t) - v0 / t - t0, where t0 = 0
if acceleration or velocity is constant, than the
average acceleration or velocity is equal to the instantaneous acceleration or velocity (linear function)
displacement is somewhat proportional to the
average velocity
an object will travel over a greater distance if it moves faster
represented by the equation x(t) = x0 + v(avg) t
where v(avg) = ½ (v0 + vt)
if the velocity vt is such as vt = v0 + at, by
substituting average velocity, the equation is: xt = x0 + [½ (v0 + vt)] t
by substituting vt, this gives the equation: xt = x0 + [½ (v0 + v0 + at)] t
this rearranges algebraically to the equation: xt = x0 + v0 t + ½ at² (position as a function of time equation)
the equation xt = x0 + v0 t + ½ at² explains
how the position of an object depends on initial velocity (v0) and acceleration (a), when acceleration is constant
v0 t = effect of initial velocity (linear function)
½ at² = effect of acceleration (quadratic function)
combining the equations for vt and xt gives the equation
v² = v0² + 2a (x - x0)
if we set the origin at the initial point (x0 = 0), it is: v² = v0² + 2ax
this equation directly relates an object’s velocity with the position at which that velocity is attained (since the variable time is eliminated, and there is only information about the distance)
distance is proportional to ∆v²