Motion

MOTION

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Class 9 Physics · Chapter 4

Describing Motion Around Us

How can a car’s motion be described? How far will it travel before stopping? Can an object accelerate even when its speed remains constant?

Motion is all around us. This chapter explains how to describe it using position, distance, displacement, speed, velocity, acceleration, graphs, and equations. Everyday examples and solved questions make the concepts easier to understand.

Think It Over

  • How much distance should be maintained from a truck ahead to avoid a collision if it suddenly applies the brakes?
  • Does this safe distance depend on the speed of the vehicle?

To answer these questions, motion must first be described precisely. The concepts in this chapter provide the tools for doing so.

What Will Be Learned?

4.1

Motion in a Straight Line

Position, reference point, distance, displacement, average speed, average velocity, and acceleration.

4.2

Graphs of Motion

Position-time and velocity-time graphs, their slopes, and the area beneath a velocity-time graph.

4.3

Kinematic Equations

Three equations for motion in a straight line with constant acceleration.

4.4

Uniform Circular Motion

Why velocity changes in circular motion even when speed is constant.

4.1 Motion in a Straight Line

When an object moves along a straight path, its motion is called linear motion. Examples include a car travelling along a straight road, a train moving on a straight track, and a ball falling vertically.

Examples illustrating rest and motion
Motion is described by tracking how an object’s position changes with time.

4.1.1 Describing Position

To describe an object’s position, a fixed point called a reference point must be chosen. The object’s distance and direction from this point specify its position.

An object is in motion when its position relative to the reference point changes with time. It is at rest when that position does not change relative to the chosen reference point.

−40 m −20 m O = 0 +20 m +40 m Positive direction → ← Negative direction
The origin is the reference point. The signs indicate direction along the straight line.
Important: Rest and motion depend on the reference point. A passenger sitting in a moving car is at rest relative to the car but is moving relative to the road.

4.1.2 Distance Travelled and Displacement

Distance travelled is the total length of the path covered by an object.

Displacement is the net change in position from the starting point to the final point, including direction.

Comparison of distance travelled and displacement
Distance measures the actual path; displacement describes the change from initial to final position.

Distance

Scalar quantity: magnitude only.

SI unit: metre (m).

It cannot be negative.

Displacement

Vector quantity: magnitude and direction.

SI unit: metre (m).

It can be zero, even when distance travelled is not zero.

Magnitude of displacement ≤ total distance travelled

Example: An athlete runs from O to A, 100 m away, and then returns 60 m towards O.

  • Total distance = 100 + 60 = 160 m.
  • Displacement = 100 − 60 = 40 m towards A.
Distance and the magnitude of displacement are equal if the object moves in one direction without turning back.

4.1.3 Average Speed and Average Velocity

Speed and velocity comparison
Speed tells how fast an object moves. Velocity also includes direction.
Average speed = Total distance travelled / Time interval Average velocity = Displacement / Time interval

Average speed is a scalar quantity. Average velocity is a vector quantity and has the direction of displacement.

Example: A swimmer covers 50 m in 50 s while swimming to the other end of a pool and back to the starting end.

Total distance = 50 m, if the trip described is the full out-and-back journey only when both lengths total 50 m. More generally, use the actual total distance supplied in a question.

Textbook example: For a total distance of 50 m and a time of 50 s, average speed is 50/50 = 1 m/s. If the swimmer returns to the starting point, displacement is zero and average velocity is 0 m/s.

4.1.4 Average Acceleration

Average acceleration describes how quickly velocity changes over a time interval.

Acceleration and changes in velocity
Acceleration may result from a change in speed, direction, or both.
a = (v − u) / t

Where:

  • u = initial velocity
  • v = final velocity
  • t = time interval
  • a = average acceleration

The SI unit of acceleration is m/s². If an object speeds up in the positive direction, acceleration is positive. If it slows down while moving in the positive direction, acceleration is negative.

An object may move very fast and still have zero acceleration if its velocity is constant. Acceleration depends on how quickly velocity changes, not on the speed alone.

Interactive Motion Simulation

Change the initial velocity and acceleration, then start the simulation. The car’s position is calculated using the equations of motion. Click the car or use Pause to pause or resume.

Position: 0 m | Velocity: 0 m/s | Time: 0 s

This is a simplified visual simulation, not a road-safety calculator.

4.2 Graphical Representation of Motion

Graphs help describe how an object’s position or velocity changes with time. Time is generally placed on the horizontal axis, while position or velocity is placed on the vertical axis.

Graphs illustrating different types of motion
Graphs represent changes in physical quantities with time.

4.2.1 Position-Time Graphs

A position-time graph shows the position of an object at different instants of time.

  • A horizontal line indicates that the object is at rest.
  • A straight inclined line indicates constant velocity.
  • A curved line indicates changing velocity and therefore accelerated motion.
  • The slope of a straight position-time graph gives velocity.
Average velocity = Change in position / Change in time

4.2.2 Velocity-Time Graphs

A velocity-time graph represents how velocity changes with time.

  • A horizontal line indicates constant velocity and zero acceleration.
  • A straight line sloping upward indicates constant positive acceleration.
  • A straight line sloping downward indicates constant negative acceleration when the object is moving in the positive direction.
  • The slope of a velocity-time graph gives acceleration.
  • The signed area under a velocity-time graph gives displacement.
Acceleration = (v − u) / t Displacement = Area under the velocity-time graph

4.3 Kinematic Equations for Constant Acceleration

For motion in a straight line with constant acceleration, initial velocity, final velocity, acceleration, time, and displacement are related by three important equations.

Equations used to describe motion
The kinematic equations connect velocity, acceleration, time, and displacement.
First equation: v = u + at Second equation: s = ut + ½at² Third equation: v² = u² + 2as

Where:

  • u is initial velocity, in m/s.
  • v is final velocity, in m/s.
  • a is constant acceleration, in m/s².
  • t is time interval, in seconds.
  • s is displacement, in metres.
Important: These equations apply to straight-line motion with constant acceleration. Use consistent SI units and signs to represent directions.

Solved Example

Question: A car moves at 15 m/s and brakes with an acceleration of −4 m/s². How far does it travel before stopping?

Given: u = 15 m/s, v = 0, a = −4 m/s².

Use the third equation:

v² = u² + 2as 0² = 15² + 2(−4)s 0 = 225 − 8s s = 225 / 8 = 28.125 m

Answer: 28.125 m.

4.4 Motion in a Plane and Uniform Circular Motion

Motion in a plane occurs in two dimensions. A vehicle overtaking another vehicle, a kicked ball, and an object moving in a circular path are examples of motion in a plane.

Uniform circular motion
Uniform circular motion: constant speed while direction changes continuously.

What Is Uniform Circular Motion?

When an object moves along a circular path with constant speed, its motion is called uniform circular motion.

Distance in one revolution = 2πR Average speed for one revolution = 2πR / T

Here, R is the radius of the circular path and T is the time taken for one complete revolution.

After one complete revolution, the object returns to its starting position. Therefore, its displacement over one complete revolution is zero and its average velocity over that interval is zero.

Key concept: In uniform circular motion, speed remains constant but velocity changes because its direction changes continuously. Therefore, the object is accelerated even though its speed does not change.

Why Does an Object Move in a Straight Line When Released?

A marble moving around the inside of a ring follows a circular path while the ring guides it. When the ring is lifted away, the marble moves along a straight line in the direction of its velocity at the instant of release, assuming other forces can be neglected.

The reason for this is explored further through Newton’s laws in the chapter on force and its effects on motion.

At a Glance: Important Formulas

QuantityFormulaSI unit
Average speedTotal distance / Timem/s
Average velocityDisplacement / Timem/s
Average acceleration(v − u) / tm/s²
First kinematic equationv = u + at—
Second kinematic equations = ut + ½at²—
Third kinematic equationv² = u² + 2as—
Circular path, one revolution2πRm
Average speed, one revolution2πR / Tm/s

Revise, Reflect, Refine — All 16 Textbook Questions

Practise first, then open the solution. All answers below follow the exercise questions and figures in the uploaded Class 9 chapter. Graph-based answers use the textbook graph values where readable.

Q1. My father went to a shop from home which is located at a distance of 250 m on a straight road. On reaching there, he discovered that he forgot to carry a cloth bag. He came home to take it, went to the shop again, bought provisions and came back home. How much was the total distance travelled by him? What was his displacement from home?

Q2. A student runs from the ground floor to the fourth floor of a school building to collect a book and then comes down to their classroom on the second floor. If the height of each floor is 3 m, find: (i) the total vertical distance travelled, and (ii) the displacement from the starting point.

Q3. A girl is riding her scooter and finds that its speedometer reading is constant. Is it possible for her scooter to be accelerating and, if so, how?

Q4. A car starts from rest and its velocity reaches 24 m/s in 6 s. Find the average acceleration and the distance travelled in these 6 s.

Q5. A motorbike moving with initial velocity 28 m/s and constant acceleration stops after travelling 98 m. Find the acceleration of the motorbike and the time taken to come to a stop.

Q6. Figure 4.27 shows a position-time graph of two objects A and B moving along parallel tracks in the same direction. Do objects A and B ever have equal velocity? Justify the answer.

A B Position (m) Time (s) 5 s 0
When position-time lines cross, the objects have the same position at that instant, not necessarily the same velocity.

Q7. Figure 4.28 shows position-time graphs of objects A and B moving in a straight line from 0 to 10 s. Choose the correct option(s).

  • (i) Their average velocities are equal because they have the same initial and final positions.
  • (ii) Their average speeds are equal because both cover equal distance in equal time.
  • (iii) Average speed of A is lower than that of B because A covers a shorter distance.
  • (iv) Average speed of A is greater than that of B.
A B Position (m) Time (s) 10
Both objects have the same initial and final positions. The curved graph changes velocity.

Q8. A truck driver travelling at 54 km/h notices a speed-limit sign of 40 km/h for trucks. The driver slows down to 36 km/h in 36 s. What distance does the truck travel during this time? Assume constant acceleration.

Q9. A car starts from rest and accelerates uniformly to 20 m/s in 5 s. It then travels at 20 m/s for 10 s and finally brakes to a stop in 6 s with uniform acceleration. Find the total distance travelled.

Q10. A bus is travelling at 36 km/h when the driver sees an obstacle 30 m ahead. The driver takes 0.5 s to react before braking. Once the brakes are applied, the velocity decreases with constant acceleration of 2.5 m/s². Will the bus stop before reaching the obstacle?

Q11. A student says, “The Earth moves around the Sun.” In this context, discuss whether an object kept on the Earth can be considered to be at rest.

Q12. The velocity-time graph from 0 s to 120 s for a cyclist is shown below. Identify the areas representing displacement (i) while the cyclist is moving with constant velocity and (ii) while the velocity is decreasing. Calculate total displacement and average acceleration during the 120 s interval.

0 3 2 20 100 120 Time (s) Velocity (m/s)
Area under the velocity-time graph gives displacement.

Q13. A girl is preparing for her first marathon by running on a straight road. Her smartwatch records the velocity-time graph shown in Figure 4.31. Estimate the distance she ran based on the graph.

0 5.0 7.0 2 4 6 Time (h) Velocity (km/h)
Schematic based on the textbook graph. Readings are approximate, so the distance is an estimate.

Q14. On entering a state highway, a car moves with constant velocity of 6 m/s for 2 minutes and then accelerates at 1 m/s² for 6 seconds. Find the displacement in the total time of 2 min 6 s using a velocity-time graph.

Q15. Two cars A and B start from rest and move in a straight line with constant acceleration. Car A reaches 5 m/s in 5 s; car B reaches 3 m/s in 10 s. Plot their velocity-time graphs on the same graph and calculate the displacement in the two time intervals.

A B 0 5 10 5 3 Time (s) Velocity (m/s)
Schematic velocity-time graph for the two cars.

Q16. Rohan studies science from 6 PM to 7:30 PM at home. Consider the tip of the minute hand of a wall clock. During the interval, calculate (i) distance travelled, (ii) displacement, (iii) average speed, and (iv) average velocity. The length of the minute hand is 7 cm.

12 2 3 4 6 8 9 10 6 PM 7:30 PM
After 90 minutes, the minute-hand tip moves from the top of the clock to the bottom.

From Describing Motion to Understanding Force

This chapter has established the language of motion: position, displacement, velocity, acceleration, graphs, and equations. These tools tell us how an object moves and how its motion changes.

The natural next question is: What causes a change in velocity? Why does a ball accelerate when kicked, why does a vehicle slow down when brakes are applied, and why does a moving object tend to continue moving in the absence of a net force?

The companion chapter on Force and How Forces Affect Motion connects these ideas through Newton’s laws. In particular, Newton’s Second Law links net force to acceleration:

Fnet = ma

The acceleration studied in this chapter is therefore the bridge between describing motion and explaining its cause. With both chapters together, it becomes easier to understand everyday motion and solve physics numericals.

Revision tip: Before practising force numericals, revise the meaning of velocity, acceleration, graph slopes, and the equations of motion from this chapter.

Class 9 Physics · Chapter 4 — Describing Motion Around Us
Understand the motion. Read the graph. Apply the formula. Solve with confidence.

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