EAPCET Physics · Intermediate first year

Motion in a Straight Line

Motion in a Straight Line describes motion in one dimension: displacement, velocity and acceleration, the equations of uniformly accelerated motion, graphs and relative velocity.

Subject
Physics
Taught in
Intermediate first year
Physics in the paper
40 of 160 questions

Key formulas and results

  • v=u+atv = u + at, s=ut+12at2s = ut + \tfrac{1}{2}at^{2}, v2=u2+2asv^{2} = u^{2} + 2as
  • Distance covered in the nth second: sn=u+a2(2n−1)s_{n} = u + \frac{a}{2}(2n - 1)
  • Displacement = area under the velocity–time graph
  • Acceleration = slope of the velocity–time graph
  • Relative velocity of A with respect to B: vAB=vA−vBv_{AB} = v_{A} - v_{B}
  • Velocity = slope of the position–time graph
  • Change in velocity = area under the acceleration–time graph
  • Acceleration in terms of position: a=vdvdxa = v\frac{dv}{dx}
  • Area under the acceleration–position graph =v2−u22= \frac{v^{2} - u^{2}}{2}
  • Distance fallen in the last second of a free fall lasting TT seconds: 12gT2−12g(T−1)2=g(T−12)\tfrac{1}{2}gT^{2} - \tfrac{1}{2}g(T - 1)^{2} = g\left(T - \tfrac{1}{2}\right)
  • Bullet and planks: if a bullet loses 1/n1/n of its speed in one plank, it stops after n22n−1\frac{n^{2}}{2n - 1} identical planks
  • If a bullet’s speed falls to u/nu/n after penetrating a distance xx, it goes a further xn2−1\frac{x}{n^{2} - 1} before stopping

What this chapter covers

  • Position, displacement and distance
  • Velocity and acceleration
  • Equations of uniformly accelerated motion
  • Motion graphs
  • Free fall
  • Relative velocity

How it is usually asked

  • Apply the equations of motion
  • Read displacement or acceleration from a graph
  • Free-fall problems
  • Relative velocity in one dimension

Understanding Motion in a Straight Line

In one dimension, position is measured from a chosen origin along a line, and the sign tells you the direction. Displacement is the change in position, while distance is the total path length, so the two differ whenever the body turns back. Velocity is the rate of change of displacement and acceleration is the rate of change of velocity; both can be positive, negative or zero.

When acceleration is constant, three equations connect u, v, a, s and t: v = u + at, s = ut + ½at² and v² = u² + 2as. Free fall is the special case a = g directed downwards. Graphs carry the same information: the slope of an x–t graph is velocity, the slope of a v–t graph is acceleration, and the area under a v–t graph is displacement.

EAPCET questions usually combine one equation of motion with a unit conversion, a graph reading, the distance covered in the nth second, or a relative-velocity idea. Before choosing an equation, list the three known quantities and the one you want; each equation leaves out one of u, v, a, s and t, so pick the one that leaves out the quantity you neither know nor need.

Worked example

EAPCET-style question

A car moving at 72 km/h is brought to rest with uniform retardation in 4 s. The distance it covers while stopping is

  1. (1)40 m
  2. (2)80 m
  3. (3)144 m
  4. (4)20 m

Solution

  1. Convert the speed: 72 km/h=72×518=20 m/s72\ \text{km/h} = 72 \times \tfrac{5}{18} = 20\ \text{m/s}.
  2. Retardation: a=0−204=−5 m/s2a = \frac{0 - 20}{4} = -5\ \text{m/s}^{2}.
  3. Use v2=u2+2asv^{2} = u^{2} + 2as: 0=202+2(−5)s0 = 20^{2} + 2(-5)s.
  4. s=400/10=40 ms = 400/10 = 40\ \text{m} (check: average speed 10 m/s×4 s=40 m10\ \text{m/s} \times 4\ \text{s} = 40\ \text{m}).

Answer: 40 m

Shortcuts and results to remember

  • For uniform acceleration, average velocity =u+v2= \frac{u + v}{2}, so you can skip the area calculation on a straight-line v–t graph.
  • The equations of motion need constant acceleration; when a body reverses direction, split the motion at the turning point (v=0v = 0) to find distance.
  • For two bodies in free fall, relative acceleration is zero, so time to meet = separation / relative velocity.
  • If a stone is dropped and another is thrown down with speed uu from the same point xx seconds later, and both land together: 12gt2=u(t−x)+12g(t−x)2\tfrac{1}{2}gt^{2} = u(t - x) + \tfrac{1}{2}g(t - x)^{2}.

More practice questions

Practice question 1

A ball is thrown vertically upward with a speed of 40 m/s. The distance it covers in the first 5 s is (g=10 m/s2g = 10\ \text{m/s}^{2})

  1. (1)75 m
  2. (2)80 m
  3. (3)85 m
  4. (4)125 m

Solution

  1. Time to reach the top =u/g=40/10=4 s= u/g = 40/10 = 4\ \text{s}
  2. Height reached =u22g=160020=80 m= \frac{u^{2}}{2g} = \frac{1600}{20} = 80\ \text{m}
  3. In the 5th second it falls from rest: 12×10×12=5 m\tfrac{1}{2} \times 10 \times 1^{2} = 5\ \text{m}
  4. Distance =80+5=85 m= 80 + 5 = 85\ \text{m} (displacement is only 75 m)

Answer: 85 m

Practice question 2

A particle starts with velocity 12 m/s and has a constant acceleration of 2 m/s22\ \text{m/s}^{2} opposite to its velocity. The distance it travels in the first 8 s is

  1. (1)32 m
  2. (2)36 m
  3. (3)40 m
  4. (4)48 m

Solution

  1. It stops when 0=12−2t0 = 12 - 2t, at t=6 st = 6\ \text{s}
  2. Distance up to the stop: 1222×2=36 m\frac{12^{2}}{2 \times 2} = 36\ \text{m}
  3. In the next 2 s it moves back: 12×2×22=4 m\tfrac{1}{2} \times 2 \times 2^{2} = 4\ \text{m}
  4. Distance =36+4=40 m= 36 + 4 = 40\ \text{m} (displacement = 32 m)

Answer: 40 m

Common mistakes to avoid

  • Using speeds in km/h inside the equations of motion — multiply by 5/18 to convert to m/s first.
  • Treating distance and displacement as equal when the body reverses direction — split the motion at the point where v = 0.
  • Taking g as positive for an upward-thrown body while also taking upward as positive — with upward positive, a = −g.
  • Applying the constant-acceleration equations when acceleration varies with time — integrate a(t) or use the graph instead.

How to prepare it

Fix a sign convention at the start and keep it — most errors in this chapter are sign errors.

Once the formulas feel familiar, test them the way the exam does: practise Motion in a Straight Line questions chapter-wise, then attempt a full previous year paper to see whether it holds up under a 3-hour timer.

Related Physics chapters

See every chapter in the EAPCET Physics syllabus.

Practise Motion in a Straight Line chapter-wise

Chapter-wise quizzes show exactly which topics in this chapter you still get wrong — before a full paper does.

Frequently asked questions

Is Motion in a Straight Line part of the EAPCET Physics syllabus?
Yes. Motion in a Straight Line is taught in Intermediate first year Physics, and the EAPCET Engineering syllabus is based on the Intermediate first- and second-year syllabus. Check the official notification each year for any changes.
How should I prepare Motion in a Straight Line for EAPCET?
Fix a sign convention at the start and keep it — most errors in this chapter are sign errors.
How many Physics questions are there in EAPCET?
40 of the 160 questions in the Engineering paper are Physics, spread across 30 chapters.
What mistakes do students make in Motion in a Straight Line?
Using speeds in km/h inside the equations of motion — multiply by 5/18 to convert to m/s first. Treating distance and displacement as equal when the body reverses direction — split the motion at the point where v = 0. Taking g as positive for an upward-thrown body while also taking upward as positive — with upward positive, a = −g. Applying the constant-acceleration equations when acceleration varies with time — integrate a(t) or use the graph instead.