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ICSE • Class 9 • Science • Ch 2
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Motion in One Dimension

In ICSE Class 9 Physics, "Motion in One Dimension" (Rectilinear Kinematics) provides the rigorous mathematical framework for describing the translational motion of an object along a single straight line without considering the forces causing that motion. The chapter begins with the foundational distinction between Scalar Quantities (having only magnitude, such as distance, speed, mass) and Vector Quantities (possessing both magnitude and direction and obeying vector addition, such as displacement, velocity, acceleration). The curriculum contrasts Distance ($s$, the total path length traversed, $s \ge 0$) with Displacement ($\vec{s}$, the shortest directed vector from the initial to final position, $|\vec{s}| \le s$). Velocity ($\vec{v} = \frac{d\vec{s}}{dt}$) and Acceleration ($\vec{a} = \frac{d\vec{v}}{dt}$, the rate of change of velocity) are rigorously analyzed. The heart of the chapter develops kinematic graphs: (1) Displacement-Time ($s-t$) Graphs, where the slope represents velocity ($\text{Slope} = \frac{\Delta s}{\Delta t} = v$); (2) Velocity-Time ($v-t$) Graphs, where the slope represents acceleration ($\text{Slope} = a$) and the area under the curve represents total displacement ($\text{Area} = s$); and (3) Acceleration-Time ($a-t$) Graphs. For uniformly accelerated rectilinear motion, students derive the three foundational kinematic equations both analytically and graphically: $v = u + at$, $s = ut + \frac{1}{2}at^2$, and $v^2 = u^2 + 2as$, as well as vertical motion under gravity ($a = \pm g$).

The Bugatti Chiron Braking Paradox: How Area Under a Graph Can Stop a 400 km/h Bullet on Wheels

Imagine you are behind the wheel of a Bugatti Chiron hypercar roaring down a runway at an astonishing 400 kilometers per hour ($111.1\text{ meters per second}$)—faster than a passenger jet at takeoff. Suddenly, you slam on the carbon-ceramic brakes with full force. Decelerating uniformly at $-10\text{ m/s}^2$, how much distance will you cover before coming to a dead stop? A novice driver might try complicated arithmetic, but a physicist looks at a simple Velocity-Time ($v-t$) graph! On the vertical axis, velocity drops from $111.1\text{ m/s}$ to $0$ in $11.1\text{ seconds}$. The shape formed under the line is a crisp, clean right-angled triangle! The base is $11.1\text{ seconds}$, the height is $111.1\text{ m/s}$. The area of that triangle—$\frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times 11.1 \times 111.1$—reveals the exact stopping distance: $617\text{ meters}$! Without calculating a single step of calculus, the geometry of graphs unlocks the physics of speed, distance, and acceleration. Let us master the laws of motion in one dimension!

Why This Chapter Matters

Kinematics is the bedrock of automotive crash safety systems, train braking distances, roller coaster loops, rocket trajectory telemetry, and athletic sports biomechanics.

Before You Begin (Prerequisites)

  • Concept of reference frame, position, and Cartesian coordinate axes from Mathematics Chapter 22.
  • Linear equations and basic algebra.

What You Will Learn (Core Objectives)

  • Differentiate clearly between scalar and vector quantities, distance and displacement, speed and velocity.
  • Distinguish between uniform and non-uniform motion, uniform velocity, and instantaneous velocity.
  • Define acceleration and retardation (deceleration) with correct SI units ($\text{m/s}^2$).
  • Extract velocity from the slope of a displacement-time graph and acceleration from the slope of a velocity-time graph.
  • Prove that the area under a velocity-time graph represents the total displacement traveled.
  • Derive and apply the three equations of uniformly accelerated motion: $v = u + at, s = ut + \frac{1}{2}at^2, v^2 = u^2 + 2as$.

Chapter Roadmap & Progression

1 1. Scalars, Vectors, Distance & Dis...
2 2. Speed, Velocity and Acceleration
3 3. Graphical Analysis of Motion
4 4. Derivation of the Equations of M...
5 5. Worked ICSE Problem Archetypes

Complete Concept Guide (100% Curriculum Coverage)

1. Scalars, Vectors, Distance & Displacement

Kinematic Terminology
A. Scalars vs Vectors:
  • Scalar: Completely specified by magnitude and unit only. Examples: Mass ($5\text{ kg}$), Distance ($20\text{ m}$), Speed ($15\text{ m/s}$), Time ($10\text{ s}$), Work, Energy.
  • Vector: Requires magnitude, unit, and a specific spatial direction. Examples: Displacement ($20\text{ m East}$), Velocity ($15\text{ m/s North}$), Acceleration, Force, Weight, Momentum.
B. Distance vs Displacement:
FeatureDistance ($s$)Displacement ($\vec{s}$)
DefinitionActual total path length traversed by an objectShortest directed straight-line distance from initial to final position
NatureScalar quantity (always positive or zero: $s \ge 0$)Vector quantity (can be positive, zero, or negative)
Path DependenceDepends on the actual route takenIndependent of path; depends strictly on initial & final points
Round TripFor a closed round trip: $\text{Distance} > 0$For a closed round trip: $\mathbf{\text{Displacement} = 0}$
Magnitude Relation$\mathbf{\text{Distance} \ge |\text{Displacement}|}$$|\vec{s}| \le s$ (Equality holds strictly for straight-line unidirectional motion)

2. Speed, Velocity and Acceleration

Rates of Motion
A. Speed and Velocity:
  • Speed ($v$): Rate of change of distance: $\text{Speed} = \frac{\text{Total Distance}}{\text{Time taken}}$ (SI unit: $\text{m/s}$ or $\text{m}\cdot\text{s}^{-1}$).
  • Velocity ($\vec{v}$): Rate of change of displacement: $\vec{v} = \frac{\text{Displacement}}{\text{Time taken}}$.
  • Average Velocity: $$\mathbf{v_{\text{avg}} = \frac{\text{Total Displacement}}{\text{Total Time Taken}}}$$ For uniformly changing velocity: $v_{\text{avg}} = \frac{u + v}{2}$.
B. Acceleration and Retardation:
  • Acceleration ($a$): Rate of change of velocity with time: $$\mathbf{a = \frac{v - u}{t} = \frac{\text{Change in Velocity}}{\text{Time Taken}}}$$ SI Unit: $\mathbf{\text{m/s}^2}$ or $\text{m}\cdot\text{s}^{-2}$.
  • Retardation / Deceleration: Negative acceleration ($a < 0$) when the speed of an object decreases with time (brakes applied).
  • Acceleration due to Gravity ($g$): The uniform downward acceleration experienced by a freely falling body under gravity alone: $g \approx 9.8\text{ m/s}^2$ (or $10\text{ m/s}^2$).

3. Graphical Analysis of Motion

Kinematic Graphs
1. Displacement-Time ($s-t$) Graph:
  • Slope: The slope of the tangent represents Velocity: $$\text{Slope} = \frac{\Delta s}{\Delta t} = v$$
  • Horizontal line (slope $= 0$) $\implies$ Object is at rest ($v = 0$).
  • Straight sloping line (constant slope) $\implies$ Uniform velocity ($a = 0$).
  • Curved line (changing slope) $\implies$ Non-uniform velocity (accelerated motion).
2. Velocity-Time ($v-t$) Graph:
  • Slope: The slope represents Acceleration: $$\text{Slope} = \frac{\Delta v}{\Delta t} = a$$
  • Area: The area enclosed between the $v-t$ curve and the time axis represents the Displacement ($s$): $$\mathbf{\text{Area under } v-t \text{ graph} = \text{Displacement } (s)}$$

4. Derivation of the Equations of Motion

The Three Kinematic Equations
Graphical Derivation from a Velocity-Time Graph:

Consider a body moving with initial velocity $u$ at $t = 0$. Under uniform acceleration $a$, its velocity increases to $v$ in time $t$.

Plot a $v-t$ graph: Point $A(0, u)$ to Point $B(t, v)$. Let $C(t, 0)$ and $O(0, 0)$ be on the time axis. Draw $AD \parallel OC$ meeting $BC$ at $D$.

Equation 1: $v = u + at$
$$\text{Slope of } AB = \text{Acceleration } (a) = \frac{BD}{AD} = \frac{v - u}{t}$$ $$at = v - u \implies \mathbf{v = u + at}$$
Equation 2: $s = ut + \frac{1}{2}at^2$

Total displacement $s =$ Area of trapezium $OABC =$ Area of rectangle $OADC$ $+$ Area of triangle $ABD$:

$$s = (OA \times OC) + \left(\frac{1}{2} \times AD \times BD\right)$$

Substitute $OA = u, OC = t, AD = t, BD = v - u = at$:

$$s = u \cdot t + \frac{1}{2} \cdot t \cdot (at) \implies \mathbf{s = ut + \frac{1}{2}at^2}$$
Equation 3: $v^2 = u^2 + 2as$

Displacement $s =$ Area of trapezium $OABC = \frac{1}{2} \times (\text{Sum of parallel sides}) \times \text{Perpendicular distance}$:

$$s = \frac{1}{2} (OA + BC) \times OC = \frac{1}{2} (u + v) \times t$$

From Equation 1, substitute $t = \frac{v - u}{a}$:

$$s = \frac{u + v}{2} \times \frac{v - u}{a} = \frac{v^2 - u^2}{2a}$$ $$2as = v^2 - u^2 \implies \mathbf{v^2 = u^2 + 2as}$$

5. Worked ICSE Problem Archetypes

Exemplary Solutions
Problem 1: A car starting from rest accelerates uniformly at $2\text{ m/s}^2$ for $10\text{ seconds}$. It then travels at constant speed for $20\text{ seconds}$ and is finally brought to rest in $5\text{ seconds}$ by applying brakes. Find: (i) Maximum velocity reached, (ii) Total distance traveled.

Solution:

Stage 1 (Acceleration): $u = 0, a = 2\text{ m/s}^2, t_1 = 10\text{ s}$.

$$v_{\max} = u + at_1 = 0 + 2(10) = \mathbf{20\text{ m/s}}$$ $$s_1 = ut_1 + \frac{1}{2}at_1^2 = 0 + \frac{1}{2}(2)(10^2) = 100\text{ meters}$$

Stage 2 (Constant Velocity): $v = 20\text{ m/s}, t_2 = 20\text{ s}, a = 0$.

$$s_2 = v \times t_2 = 20 \times 20 = 400\text{ meters}$$

Stage 3 (Retardation): $u = 20\text{ m/s}, v = 0, t_3 = 5\text{ s}$.

$$s_3 = \text{Average velocity} \times t_3 = \frac{20 + 0}{2} \times 5 = 10 \times 5 = 50\text{ meters}$$

Total Distance Traveled:

$$s = s_1 + s_2 + s_3 = 100 + 400 + 50 = \mathbf{550\text{ meters}}$$
Problem 2: A ball is thrown vertically upwards with a velocity of $49\text{ m/s}$. Calculate: (i) The maximum height reached, (ii) The total time taken to return to the ground (take $g = 9.8\text{ m/s}^2$).

Solution:

Initial velocity $u = 49\text{ m/s}$. At maximum height, final velocity $v = 0$. Downward acceleration $a = -g = -9.8\text{ m/s}^2$.

(i) Maximum Height ($h$):

$$v^2 = u^2 - 2gh \implies 0 = 49^2 - 2(9.8)h$$ $$19.6h = 2401 \implies h = \frac{2401}{19.6} = \mathbf{122.5\text{ meters}}$$

(ii) Time of Ascent ($t$):

$$v = u - gt \implies 0 = 49 - 9.8t \implies t = \frac{49}{9.8} = 5\text{ seconds}$$

Total time of flight $= 2 \times t_{\text{ascent}} = 2 \times 5 = \mathbf{10\text{ seconds}}$.

Key Formulas, Reactions & Definitions

First Equation of Motion
v = u + at
Velocity-time relation for uniform acceleration.
Second Equation of Motion
$$s = ut + \frac{1}{2}at^2$$
Position-time relation.
Third Equation of Motion
$$v^2 = u^2 + 2as$$
Velocity-position relation.
Motion Under Gravity
$$v = u \pm gt, \quad h = ut \pm \frac{1}{2}gt^2, \quad v^2 = u^2 \pm 2gh$$
Plus for downward, minus for upward motion.
Slope of s-t Graph
$$v = \frac{\Delta s}{\Delta t}$$
Slope of displacement-time curve gives velocity.
Area under v-t Graph
$$s = \text{Area under } v(t)$$
Area gives total displacement.

Physics: Velocity-Time Graph Derivation of Equations of Motion

Velocity-Time (v-t) Graph: Graphical Derivation of Equations of Motion Time t (s) Velocity v (m/s) O (0,0) A (u) B (v) D C (t) Area 1 (Rectangle) = u × t Area 2 (Δ) = ½ t(v - u) = ½at² BD = at AD = t Summary of Derivations: 1. Slope = a = (v - u)/t ⇒ v = u + at 2. Total Area = s = ut + ½at² 3. Eliminating t ⇒ v² = u² + 2as

Chapter Summary & 10 Key Takeaways

Takeaway 1
Scalars have magnitude only (mass, distance, speed); vectors have magnitude and direction (displacement, velocity, acceleration).
Takeaway 2
Distance is the total path length (s ≥ 0); displacement is the shortest directed vector between initial and final points.
Takeaway 3
Speed is rate of change of distance (scalar); velocity is rate of change of displacement (vector).
Takeaway 4
Acceleration is the rate of change of velocity: a = (v - u) / t (unit: m/s^2).
Takeaway 5
Negative acceleration is called deceleration or retardation.
Takeaway 6
The slope of a displacement-time graph represents velocity (v = Δs / Δt).
Takeaway 7
The slope of a velocity-time graph represents acceleration (a = Δv / Δt).
Takeaway 8
The area under a velocity-time graph represents total displacement.
Takeaway 9
The three kinematic equations for uniform acceleration are: v = u + at, s = ut + 1/2 at^2, and v^2 = u^2 + 2as.
Takeaway 10
For freely falling bodies under gravity, replace a with +g (falling down) or -g (thrown upwards).

Check Your Understanding (Diagnostic Practice Questions)

Diagnostic questions testing core conceptual clarity. Answers are hidden initially — solve each problem first, then click to reveal the step-by-step verified solution.

1
A body moves along a circular path of radius $r$. Find the distance traveled and displacement when it completes: (i) Half a revolution, (ii) One full revolution.
Reveal Answer & Explanation
Answer:

• (i) Half a revolution:
- Distance: Half the circumference $= \frac{1}{2}(2\pi r) = \mathbf{\pi r}$.
- Displacement: The body moves from one end of the diameter to the opposite end $\implies$ length of the diameter $= \mathbf{2r}$ (directed from start to finish).
• (ii) One full revolution:
- Distance: Complete circumference $= \mathbf{2\pi r}$.
- Displacement: The body returns to its exact starting point $\implies \mathbf{\text{Displacement} = 0}$.


For half a circle, distance is πr, displacement is diameter 2r. For full circle, displacement is 0.
2
Can a body have a constant speed but a variable velocity? Give an example.
Reveal Answer & Explanation
Answer:

• Yes. Velocity is a vector quantity having both magnitude (speed) and direction. If the direction changes while speed remains constant, the velocity is variable.
• Example: An object moving in a uniform circular motion (e.g., a satellite orbiting Earth at constant speed $v$). Its speed is constant, but its direction of motion changes continuously at every point along the tangent, producing a continuously changing velocity and a centripetal acceleration.


Yes. Uniform circular motion has constant speed but continuously changing direction of velocity.
3
What physical quantity is represented by: (i) The slope of a displacement-time graph, (ii) The slope of a velocity-time graph, (iii) The area under a velocity-time graph?
Reveal Answer & Explanation
Answer:

• (i) Slope of $s-t$ graph: $\frac{\Delta s}{\Delta t} = \mathbf{\text{Velocity}}$.
• (ii) Slope of $v-t$ graph: $\frac{\Delta v}{\Delta t} = \mathbf{\text{Acceleration}}$.
• (iii) Area under $v-t$ graph: $\int v \, dt = \mathbf{\text{Displacement}}$ (distance traveled).


(i) Velocity, (ii) Acceleration, (iii) Displacement.
4
A car moving with an initial speed of $72\text{ km/h}$ is brought to rest in $5\text{ seconds}$ by applying brakes. Calculate the retardation and the distance traveled before coming to a stop.
Reveal Answer & Explanation
Answer:

• Convert speed to SI units ($1\text{ km/h} = \frac{5}{18}\text{ m/s}$):

$$u = 72 \times \frac{5}{18} = 20\text{ m/s}$$


Final velocity $v = 0$, Time $t = 5\text{ s}$.
• Retardation:

$$a = \frac{v - u}{t} = \frac{0 - 20}{5} = -4\text{ m/s}^2 \implies \mathbf{\text{Retardation} = 4\text{ m/s}^2}$$


• Distance Traveled ($s$):

$$s = ut + \frac{1}{2}at^2 = (20 \times 5) + \frac{1}{2}(-4)(5^2) = 100 - 50 = \mathbf{50\text{ meters}}$$

(Or using $v^2 = u^2 + 2as \implies 0 = 400 - 8s \implies s = 50\text{ m}$).


u = 20 m/s. a = (0 - 20)/5 = -4 m/s^2 (retardation = 4 m/s^2). Distance = 20*5 - (1/2)*4*25 = 50 m.
5
A pebble dropped from the top of a cliff reaches the valley floor in $4\text{ seconds}$. Find the height of the cliff (take $g = 9.8\text{ m/s}^2$).
Reveal Answer & Explanation
Answer: • Initial velocity $u = 0$ (dropped from rest). Time $t = 4\text{ s}$, $a = +g = 9.8\text{ m/s}^2$.
• Using the second equation of motion under gravity:
$$h = ut + \frac{1}{2}gt^2$$
$$h = 0(4) + \frac{1}{2}(9.8)(4^2) = 4.9 \times 16 = \mathbf{78.4\text{ meters}}$$
h = (1/2) * g * t^2 = 4.9 * 16 = 78.4 m.
6
State the condition under which the magnitude of displacement equals the distance traveled.
Reveal Answer & Explanation
Answer:

• The magnitude of displacement equals the distance traveled if and only if the object moves along a straight line in a single, unchanging direction without any backtracking or turning back ($|\vec{s}| = s$).


Straight-line motion in a single unchanging direction without turning back.
7
A train starts from a station and moves with a uniform acceleration of $0.2\text{ m/s}^2$ for $2\text{ minutes}$. Find the speed acquired in $\text{km/h}$.
Reveal Answer & Explanation
Answer: • Given: $u = 0$, $a = 0.2\text{ m/s}^2$, $t = 2\text{ minutes} = 120\text{ seconds}$.
• Using $v = u + at$:
$$v = 0 + 0.2 \times 120 = 24\text{ m/s}$$
• Convert $\text{m/s}$ to $\text{km/h}$ (multiply by $\frac{18}{5}$):
$$v = 24 \times \frac{18}{5} = \frac{432}{5} = \mathbf{86.4\text{ km/h}}$$
v = 0.2 * 120 = 24 m/s. 24 * (18/5) = 86.4 km/h.
8
Explain the difference between instantaneous speed and average speed.
Reveal Answer & Explanation
Answer:

• Instantaneous Speed: The speed of a moving object at a specific, infinitesimal instant of time ($v = \lim_{\Delta t \to 0} \frac{\Delta s}{\Delta t}$). It is the value registered on a car's speedometer.
• Average Speed: The overall ratio of the total distance traveled by the object to the total time taken for the complete journey ($v_{\text{avg}} = \frac{\text{Total Distance}}{\text{Total Time}}$). It smooths out all intermediate accelerations and stops.


Instantaneous speed is speed at an exact instant (speedometer). Average speed is total distance / total time.
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