Irodov 1.18

From a vx(t) Graph to wx, x and s

$w_x=\dfrac{dv_x}{dt},\; x=\int v_x\,dt,\; s=\int |v_x|\,dt$–
(i) The Answer in One Line

$w_x$ is the slope of the $v_x$ graph: $+1,\,0,\,-1,\,+2,\,0$. The coordinate $x$ is the signed area: it peaks at $x=3$ when $t=4$, then ends at $x=0$ at $t=7$. The distance $s$ is the unsigned area: it ends at $s=6$ units.

(ii) Problem Statement

"A point travels along the $x$ axis with a velocity whose projection $v_x$ is presented as a function of time by the plot in the figure. Assuming the coordinate of the point $x=0$ at the moment $t=0$, draw the approximate time dependence plots for the acceleration $w_x$, the $x$ coordinate, and the distance covered $s$."

What this problem teaches: one velocity graph hides three more graphs. Slopes give acceleration. Areas give position. Areas counted as positive give distance.

(iii) The Big Idea in Plain Words

A point slides along a line. We are told how fast it goes at each moment. We must find how its speed changes, where it is, and how far it has walked in total.

Symbols: $t$ is time. $v_x$ is velocity along $x$ (negative means moving left). $w_x$ is acceleration, the rate at which $v_x$ changes. $x$ is the position. $s$ is the total path length.

The graph has five straight pieces, so each piece is easy:

PieceTime$v_x$$w_x$ (slope)$x$ at end$s$ at end
oa0 to 10 → 1+11/21/2
ab1 to 3stays 105/25/2
b43 to 41 → 0−133
4d4 to 60 → −2−115
d76 to 7−2 → 0+206

Shape of the plots: $w_x$ is flat steps with jumps. $x$ is smooth, with a peak at $t=4$. $s$ is smooth and never falls. After $t=7$, $w_x=0$, $x=0$ and $s=6$ stay constant.

(iv) The Solution Viewed in Each Frame

1. Ground (Lab) Frame (stationary observer)

Why: the graph was recorded by a still observer, so this is the natural frame.
Read the slopes: $w_x=+1,\,0,\,-1,\,+2,\,0$ on the five pieces.

Why: position is the signed area under the $v_x$ graph.
$x$: $\tfrac12+2+\tfrac12=3$ at $t=4$. Then $-2$ gives $1$ at $t=6$. Then $-1$ gives $0$ at $t=7$.

Why: distance ignores direction, so every area counts as positive.
$s=\tfrac12+2+\tfrac12+2+1=6$ units.

2. Centre-of-Mass Frame (origin rides on the point)

Why: for a single point, the centre of mass is the point itself.
In this frame $x'=0$ and $v'=0$ at all times, so the momentum about the centre of mass is zero trivially. The ground slides past with velocity $-v_x$.

Why: this frame accelerates, so a pseudo-force appears.
Any small object resting in it would feel $-m\,w_x$, pointing opposite to $w_x$. No such object is in the problem.

Why: undo the shift to compare with the ground.
The ground's displacement is $-x$, so the point's $x$ is its negative: $x(7)=0$. The ground's path length is the same: $s=6$.

3. Medium Frame

Does not apply. There is no water, air or other fluid in this problem. The view equals the ground frame.

What changes and what stays the same
  • Changes: the picture. In the centre-of-mass frame the point is fixed, the ground moves with $-v_x$, and a pseudo-force $-m\,w_x$ appears.
  • Same: the final answers. $x(7)=0$, $s(7)=6$, and the peak $x=3$ at $t=4$, in every frame.

(v) The Solution by Each Method

Method 1: Graph Method (areas and slopes)

  1. Why: the graph is given, so use its slopes and areas directly.
    Slopes: $w_x=+1,0,-1,+2,0$.
  2. Why: split the area into triangles and a rectangle.
    Triangle 0–1: $\tfrac12$. Rectangle 1–3: $2$. Triangle 3–4: $\tfrac12$. Triangle 4–6 (below axis): $2$. Triangle 6–7 (below axis): $1$.
  3. Why: signed sum gives $x$; unsigned sum gives $s$.
    $x=\tfrac12+2+\tfrac12-2-1=0$. $s=\tfrac12+2+\tfrac12+2+1=6$.

Method 2: Calculus Method (the book's route)

  1. Why: acceleration is the derivative of velocity.
    $w_x=\dfrac{dv_x}{dt}$ gives $+1,0,-1,+2,0$ on the five pieces.
  2. Why: integrate $v_x$ piece by piece, starting each piece where the last ended.
    0–1: $x=\tfrac{t^2}{2}$. 1–3: $x=t-\tfrac12$. 3–6: $v_x=4-t$, so $x=4t-\tfrac{t^2}{2}-5$ (gives $3$ at $t=4$, $1$ at $t=6$). 6–7: $v_x=2(t-7)$, so $x=(t-7)^2$, which is $1$ at $t=6$ and $0$ at $t=7$.
  3. Why: for $s$, integrate $|v_x|$ so it only grows.
    After $t=4$ use $|v_x|=t-4$ then $2(7-t)$. This gives $s(6)=5$ and $s(7)=6$.

Method 3: Force Method

Only partly suits this problem. No mass or forces are given, so no free-body diagram has numbers. We can still say $F=m\,w_x$, so the force is proportional to the slope. It cannot give $x$ or $s$.

Method 4: Energy Method

Does not suit this problem. Nothing is given about forces, heights or masses, and energy does not tell direction or position.

Method 5: Relative-Motion Method

The ground frame already gives the graph, so it is the shortest frame. One line: signed area $=0$, unsigned area $=6$. A moving frame would only add steps.

Fastest: Method 1 (just areas). Most reliable in an exam: Method 2 (every number comes from a formula). Both give $x(7)=0$ and $s(7)=6$.

(vi) Parameter Table

SymbolMeaningUnitLive value

(vii) Common Exam Traps

Verified: the live plots, both frames and all methods agree — $x(7)=0$, $s(7)=6$, peak $x=3$ at $t=4$ for the book values, with $v$ in units per time unit, $w$ in units per time unit squared.