Motion in a Straight Line | Class 11 Physics Notes
By ConceptScroll Team · Published on 17 July 2026 · 3 min read

Motion in a Straight Line – this guide gives you a concise, exam-ready overview of Motion in a Straight Line from Class 11 Physics, written by ConceptScroll editors and reviewed against the latest NCERT textbook.
Examples of uniformly accelerated motion
Several examples illustrate the application of kinematic equations for uniformly accelerated motion:
1. Ball thrown vertically upwards from a building (Example 2.3): A ball is thrown upwards with initial velocity v₀ = 20 m/s from a building 25 m high. Taking upward as positive and acceleration due to gravity g = 10 m/s² downward, the maximum height reached and total time before hitting the ground are calculated using kinematic equations.
2. Free fall (Example 2.4): An object falling freely under gravity with acceleration g = 9.8 m/s² downward is described. Starting from rest, its velocity, displacement, and velocity squared as functions of time are given by:
v = -g t,
y = - (1/2) g t²,
v² = -2 g y.
Graphs of acceleration, velocity, and displacement versus time are shown.
3. Galileo's law of odd numbers (Example 2.5): Galileo observed that distances fallen in successive equal time intervals by a freely falling body starting from rest are in the ratio of odd numbers 1:3:5:7... This is demonstrated by calculating distances fallen in successive intervals and showing the ratio matches odd numbers.
4. Stopping distance of vehicles (Example 2.6): When brakes are applied, the stopping distance d_v depends on initial velocity v_it and braking deceleration -α. Using v² = v₀² + 2 a x with final velocity zero, stopping distance is:
d_v = v_it² / (2 α).
This shows stopping distance increases with the square of initial velocity, important for road safety.
5. Reaction time (Example 2.7): Reaction time is the delay between perceiving a situation and responding. It can be measured by dropping a ruler and catching it, then calculating the time taken based on the distance fallen under gravity:
t_r = √(2 d / g).
For a distance d = 21 cm, reaction time is approximately 0.2 s.
📊 Diagram: Fig. 2.6 shows the vertical motion of a ball thrown upwards from a building; Fig. 2.7 shows graphs of acceleration, velocity, and displacement versus time for free fall; Table 2.2 illustrates Galileo's law of odd numbers; Fig. 2.8 shows the ruler drop experiment for reaction time.
🧪 Activity: Measuring reaction time by ruler drop experiment as described in Example 2.7.
🔗 Connection: These examples provide practical applications of kinematic equations, leading to a summary of concepts and definitions in the next section.
Table on page 8 (8×5)
| t | y | y in terms of yv [=( - 1/2) g τ2] | Distance traversed in successive intervals | Ratio of distances traversed |
|---|---|---|---|---|
| 0 | 0 | 0 | ||
| τ | -(1/2) g τ2 | yv | yv | 1 |
| 2 τ | -4(1/2) g τ2 | 4 yv | 3 yv | 3 |
| 3 τ | -9(1/2) g τ2 | 9 yv | 5 yv | 5 |
| 4 τ | -16(1/2) g τ2 | 16 yv | 7 yv | 7 |
| 5 τ | -25(1/2) g τ2 | 25 yv | 9 yv | 9 |
| 6 τ | -36(1/2) g τ2 | 36 yv | 11 yv | 11 |
Frequently asked questions
Which of the following repetitive phenomena in nature could serve as time standards in near future?
All of above
A particle executes simple harmonic motion of time period 4 seconds. After what time of it passing through the mean position, will the kinetic energy be half kinetic and half potential?
0.5 s
Identify the pair that does not have similar dimensions:
Tension and surface tension
The circumference of a circle, of diameter 2.06m, with correct number of significant figures is
6.47m
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