CLASSICAL-MECHANICS

From Secant to Tangent: Defining Velocity as a Derivative

IKey Formulas

Formula Name Description
vave=Ξ”xΞ”t=xfβˆ’xitfβˆ’tiv_{\text{ave}} = \dfrac{\Delta x}{\Delta t} = \dfrac{x_f - x_i}{t_f - t_i} Average velocity Slope of the secant line on an xx–tt graph
v(t)=lim⁑Δtβ†’0x(t+Ξ”t)βˆ’x(t)Ξ”t=dxdtv(t) = \displaystyle\lim_{\Delta t \to 0} \dfrac{x(t+\Delta t) - x(t)}{\Delta t} = \dfrac{dx}{dt} Instantaneous velocity Slope of the tangent line; the derivative of position
Ξ”x=xfβˆ’xi\Delta x = x_f - x_i Displacement Signed change in position (not distance traveled)
v(ti)+v(tf)2=vave\dfrac{v(t_i) + v(t_f)}{2} = v_{\text{ave}} Endpoint mean Equals vavev_{\text{ave}} only when v(t)v(t) is linear in tt

IIInteractive Visualizations

Visualization 1 β€” Displacement vs. Distance

On a there-and-back trip the object comes home, so does its average velocity depend on how far it went?

Visualization 2 β€” Secant Becomes Tangent

As the interval Ξ”t\Delta t shrinks to zero, what fixed value does the secant slope close in on?

πŸ’‘ This limiting slope β€” the secant slope as Ξ”tβ†’0\Delta t \to 0 β€” is the derivative dx/dtdx/dt, the instantaneous velocity v(1)v(1).

Visualization 3 β€” Average Velocity and the Midpoint

For linear v(t)v(t), where on [ti,tf][t_i, t_f] does the instantaneous velocity equal the average velocity?

πŸ’‘ The midpoint match is special to linear v(t)v(t); once v(t)v(t) bends, the parallel-tangent point drifts off the midpoint and the endpoint-velocity mean no longer equals vavev_{\text{ave}}.

IIIQuiz Questions

Question 1

An object moves 55 m in the +x+x direction, then 55 m back to its starting point. The round trip takes 22 s.

What is the object's average velocity over the round trip?

βœ… Correct! Net displacement is zero, so the average velocity is zero.

❌ Not quite. That is the average speed (distance / time), not the average velocity, which uses displacement.

❌ Not quite. Average velocity = displacement / time, and the displacement of a round trip is zero.

Show solution

Solution:

Average velocity uses displacement, not distance. The object returns to its starting point, so the net displacement is

Ξ”x=xfβˆ’xi=0.\Delta x = x_f - x_i = 0.

Therefore

vave=Ξ”xΞ”t=02Β s=0Β m/s.v_{\text{ave}} = \frac{\Delta x}{\Delta t} = \frac{0}{2\ \text{s}} = 0\ \text{m/s}.

The total distance is 1010 m and the average speed is 55 m/s, but speed and velocity are different quantities. The answer is 0 m/s.

Question 2

On a position-versus-time graph, the average velocity over an interval is represented geometrically by which of the following?

βœ… Correct! Average velocity is rise over run β€” the secant slope.

❌ Not quite. The tangent slope is the instantaneous velocity. The average velocity is the secant slope.

❌ Not quite. Average velocity = Ξ”x/Ξ”t = rise/run, which is the slope of the secant line.

Show solution

Solution:

Average velocity is

vave=Ξ”xΞ”t=riserun,v_{\text{ave}} = \frac{\Delta x}{\Delta t} = \frac{\text{rise}}{\text{run}},

which is exactly the slope of the straight line β€” the secant β€” joining the two endpoints (ti,x(ti))(t_i, x(t_i)) and (tf,x(tf))(t_f, x(t_f)) on the xx–tt graph.

  • The slope of the tangent at a single point is the instantaneous velocity, not the average.
  • The area under an xx–tt curve has no direct velocity meaning.

The answer is the slope of the secant line connecting the two endpoints.

Question 3

For the position function x(t)=x0+12b t2x(t) = x_0 + \tfrac{1}{2} b\, t^2, the limit definition of the derivative gives the instantaneous velocity v(t)=b tv(t) = b\,t.

If b=4Β m/s2b = 4\ \text{m/s}^2, what is the instantaneous velocity at t=3t = 3 s?

βœ… Correct! v(t) = bΒ·t = 4 Γ— 3 = 12 m/s.

❌ Not quite. 18 comes from ½ b t² (the position). Velocity is v(t) = b·t.

❌ Not quite. Use v(t) = b·t with b = 4 and t = 3, giving 12 m/s.

Show solution

Solution:

From the limit definition,

v(t)=lim⁑Δtβ†’0x(t+Ξ”t)βˆ’x(t)Ξ”t=b t.v(t) = \lim_{\Delta t \to 0} \frac{x(t+\Delta t) - x(t)}{\Delta t} = b\,t.

Substituting b=4Β m/s2b = 4\ \text{m/s}^2 and t=3t = 3 s:

v(3)=b t=(4)(3)=12Β m/s.v(3) = b\,t = (4)(3) = 12\ \text{m/s}.

A common trap is to plug into 12b t2\tfrac{1}{2} b\,t^2 (the position) or to forget the factor of tt. The velocity is v(t)=b tv(t) = b\,t, so the answer is 12 m/s.

Question 4

True or False: The arithmetic mean of the endpoint velocities, v(ti)+v(tf)2\dfrac{v(t_i) + v(t_f)}{2}, always equals the average velocity vave=Ξ”xΞ”tv_{\text{ave}} = \dfrac{\Delta x}{\Delta t} for any motion.

βœ… Correct! The endpoint-mean identity holds only for linear v(t), not for every motion.

❌ Not quite. It is true only when v(t) is linear in t. In general, v_ave ≑ Ξ”x/Ξ”t.

❌ Not quite. Try again β€” the hints above can help.

Show solution

Solution:

The statement is False. The identity

v(ti)+v(tf)2=vave\frac{v(t_i) + v(t_f)}{2} = v_{\text{ave}}

holds only when v(t)v(t) is a linear function of time, as in x(t)=x0+v0t+12b t2x(t) = x_0 + v_0 t + \tfrac{1}{2} b\, t^2, where v(t)=v0+b tv(t) = v_0 + b\,t. In that special case both sides reduce to v0+12b (tf+ti)v_0 + \tfrac{1}{2} b\,(t_f + t_i).

For any nonlinear velocity function, the arithmetic mean of the endpoint velocities will not match the true average velocity. The reliable definition is always

vave≑ΔxΞ”t.v_{\text{ave}} \equiv \frac{\Delta x}{\Delta t}.

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