Chapter Notes

Motion

15 min read

Motion

In physics, motion describes a change in an object's position over time. We see it everywhere: birds flying, cars moving, and even planets orbiting the sun. An object that is not changing its position is said to be at rest.

However, motion is relative. It depends on the observer's point of view.

Example
Imagine you are a passenger on a moving bus. To you, the person sitting next to you appears to be at rest. But to a person standing on the roadside, both you and the other passenger are in motion. This shows that an object can appear to be moving for one person and stationary for another.

Motion can be simple, like moving in a straight line, or complex, like a combination of rotating and vibrating. In this chapter, we will learn how to describe motion, especially along a straight line and in a circle, using simple equations and graphs.

Describing Motion

To describe where an object is, we need a point of reference. This fixed point is called the origin. We describe the object's position relative to this origin.

Example
If we say a school is 2 km north of a railway station, we are using the railway station as the reference point, or origin, to describe the school's location.

Motion along a straight line

The simplest type of motion is movement along a straight line. To understand this, we use two key physical quantities: distance and displacement.

Distance is the total path length an object covers. It is a scalar quantity, meaning it only has a numerical value, or magnitude, and does not require a direction.

Displacement is the shortest distance measured from the initial position to the final position of an object. It is a vector quantity, meaning it includes both magnitude and direction.

Let's consider an object moving along a straight path. It starts at the origin O, travels to point A, and then returns to point C.

  • The distance covered is the total path length: (Path OA) + (Path AC).
  • The displacement is the shortest distance between the start (O) and end (C) points, which is simply the length OC.
Note
The magnitude of the displacement is not always equal to the distance travelled. For example, if an object travels from O to A (60 km) and back to O, the total distance is 60 km+60 km=120 km60 \text{ km} + 60 \text{ km} = 120 \text{ km}. However, since the final position is the same as the initial position, the displacement is zero. The magnitude of displacement can only be equal to the distance if the object travels in a straight line without changing direction.

Uniform motion and non-UNIFORM MOTION

We can classify motion based on how an object's speed changes over time.

  • Uniform Motion: An object is in uniform motion if it travels equal distances in equal intervals of time. For example, a car moving at a constant 5 meters every second.
  • Non-uniform Motion: An object is in non-uniform motion if it travels unequal distances in equal intervals of time. For instance, a car moving in city traffic or a person jogging in a park will speed up and slow down.

Measuring the Rate of Motion

To measure how fast or slow an object is moving, we use the concept of speed.

Speed is the distance an object travels per unit of time.

  • The SI unit for speed is metre per second (m s1\text{m s}^{-1} or m/s).
  • Other common units include centimetre per second (cm s1\text{cm s}^{-1}) and kilometre per hour (km h1\text{km h}^{-1}).

The formula for speed is: v=stv = \frac{s}{t} where vv is speed, ss is distance, and tt is time.

In most real-world situations, objects are in non-uniform motion. For these cases, we describe the rate of motion using average speed.

Average speed is the total distance travelled divided by the total time taken. average speed=Total distance travelledTotal time taken\text{average speed} = \frac{\text{Total distance travelled}}{\text{Total time taken}}

Example
Example An object travels 16 m in 4 s and then another 16 m in 2 s. What is the average speed of the object?

Given

  • Distance 1, s1=16s_1 = 16 m
  • Time 1, t1=4t_1 = 4 s
  • Distance 2, s2=16s_2 = 16 m
  • Time 2, t2=2t_2 = 2 s

To Find

The average speed of the object.

Formula

Average speed=Total distance travelledTotal time taken\text{Average speed} = \frac{\text{Total distance travelled}}{\text{Total time taken}}

Solution

Total distance travelled = 16 m+16 m=32 m16 \text{ m} + 16 \text{ m} = 32 \text{ m} Total time taken = 4 s+2 s=6 s4 \text{ s} + 2 \text{ s} = 6 \text{ s}

Substitute the values into the formula: Average speed=32 m6 s=5.33 m s1\text{Average speed} = \frac{32 \text{ m}}{6 \text{ s}} = 5.33 \text{ m s}^{-1}

Final Answer The average speed of the object is 5.33 m s15.33 \text{ m s}^{-1}.

Speed with direction

To provide a more complete description of motion, we need to specify its direction along with its speed. This quantity is called velocity.

Velocity is the speed of an object moving in a definite direction.

  • The velocity of an object can be uniform or variable. It can be changed by changing the object's speed, its direction of motion, or both.
  • The units for speed and velocity are the same (m s1\text{m s}^{-1}).

When an object's velocity is changing at a uniform rate, its average velocity is the arithmetic mean of its initial and final velocities. average velocity=initial velocity+final velocity2\text{average velocity} = \frac{\text{initial velocity} + \text{final velocity}}{2} Mathematically, this is written as: vav=u+v2v_{av} = \frac{u+v}{2} where vavv_{av} is the average velocity, uu is the initial velocity, and vv is the final velocity.

Example
Example The odometer of a car reads 2000 km at the start of a trip and 2400 km at the end of the trip. If the trip took 8 h, calculate the average speed of the car in km h1\text{km h}^{-1} and m s1\text{m s}^{-1}.

Given

  • Initial odometer reading = 2000 km
  • Final odometer reading = 2400 km
  • Time elapsed, t=8t = 8 h

To Find

The average speed in km h1\text{km h}^{-1} and m s1\text{m s}^{-1}.

Formula

vav=stv_{av} = \frac{s}{t}

Solution

First, calculate the total distance covered: Distance, s=2400 km2000 km=400 kms = 2400 \text{ km} - 2000 \text{ km} = 400 \text{ km}

Now, calculate the average speed in km h1\text{km h}^{-1}: vav=400 km8 h=50 km h1v_{av} = \frac{400 \text{ km}}{8 \text{ h}} = 50 \text{ km h}^{-1}

To convert this to m s1\text{m s}^{-1}, we use the conversion factors 1 km=1000 m1 \text{ km} = 1000 \text{ m} and 1 h=3600 s1 \text{ h} = 3600 \text{ s}: 50kmh×1000 m1 km×1 h3600 s=13.9 m s150 \frac{\text{km}}{\text{h}} \times \frac{1000 \text{ m}}{1 \text{ km}} \times \frac{1 \text{ h}}{3600 \text{ s}} = 13.9 \text{ m s}^{-1}

Final Answer The average speed of the car is 50 km h150 \text{ km h}^{-1} or 13.9 m s113.9 \text{ m s}^{-1}.

Example
Example Usha swims in a 90 m long pool. She covers 180 m in one minute by swimming from one end to the other and back along the same straight path. Find the average speed and average velocity of Usha.

Given

  • Total distance covered = 180 m
  • Total time taken = 1 minute = 60 s
  • Length of pool = 90 m

To Find

Average speed and average velocity.

Formula

Average speed=Total distance coveredTotal time taken\text{Average speed} = \frac{\text{Total distance covered}}{\text{Total time taken}} Average velocity=DisplacementTotal time taken\text{Average velocity} = \frac{\text{Displacement}}{\text{Total time taken}}

Solution

Average Speed: Average speed=180 m60 s=3 m s1\text{Average speed} = \frac{180 \text{ m}}{60 \text{ s}} = 3 \text{ m s}^{-1}

Average Velocity: Usha starts at one end and swims to the other and back. Her final position is the same as her initial position. Therefore, her displacement is 0 m. Average velocity=0 m60 s=0 m s1\text{Average velocity} = \frac{0 \text{ m}}{60 \text{ s}} = 0 \text{ m s}^{-1}

Final Answer The average speed of Usha is 3 m s13 \text{ m s}^{-1} and her average velocity is 0 m s10 \text{ m s}^{-1}.

Rate of Change of Velocity

In non-uniform motion, velocity changes with time. The rate at which velocity changes is described by another physical quantity called acceleration.

Acceleration is the change in the velocity of an object per unit time. acceleration=change in velocitytime taken\text{acceleration} = \frac{\text{change in velocity}}{\text{time taken}} If an object's velocity changes from an initial value uu to a final value vv in time tt, the acceleration aa is: a=vuta = \frac{v-u}{t}

  • The SI unit of acceleration is metre per second squared (m s2\text{m s}^{-2}).
  • Acceleration is positive if it is in the direction of velocity (speeding up).
  • Acceleration is negative if it is opposite to the direction of velocity (slowing down).

Uniform Acceleration: The acceleration is uniform if an object's velocity changes by equal amounts in equal intervals of time. A freely falling body is an example of uniformly accelerated motion.

Non-uniform Acceleration: The acceleration is non-uniform if the velocity changes at a non-uniform rate.

Example
Example Starting from a stationary position, Rahul paddles his bicycle to attain a velocity of 6 m s16 \text{ m s}^{-1} in 30 s. Then he applies brakes such that the velocity of the bicycle comes down to 4 m s14 \text{ m s}^{-1} in the next 5 s. Calculate the acceleration of the bicycle in both the cases.

Given

Case 1:

  • Initial velocity, u=0 m s1u = 0 \text{ m s}^{-1} (stationary)
  • Final velocity, v=6 m s1v = 6 \text{ m s}^{-1}
  • Time, t=30t = 30 s

Case 2:

  • Initial velocity, u=6 m s1u = 6 \text{ m s}^{-1}
  • Final velocity, v=4 m s1v = 4 \text{ m s}^{-1}
  • Time, t=5t = 5 s

To Find

The acceleration, aa, in both cases.

Formula

a=vuta = \frac{v-u}{t}

Solution

(i) First Case (Speeding up) a=6 m s10 m s130 s=630 m s2=0.2 m s2a = \frac{6 \text{ m s}^{-1} - 0 \text{ m s}^{-1}}{30 \text{ s}} = \frac{6}{30} \text{ m s}^{-2} = 0.2 \text{ m s}^{-2} Answer for part (i) = 0.2 m s20.2 \text{ m s}^{-2}


(ii) Second Case (Slowing down) a=4 m s16 m s15 s=25 m s2=0.4 m s2a = \frac{4 \text{ m s}^{-1} - 6 \text{ m s}^{-1}}{5 \text{ s}} = \frac{-2}{5} \text{ m s}^{-2} = -0.4 \text{ m s}^{-2} Answer for part (ii) = 0.4 m s2-0.4 \text{ m s}^{-2}


Final Answer The acceleration of the bicycle in the first case is 0.2 m s20.2 \text{ m s}^{-2} and in the second case, it is 0.4 m s2-0.4 \text{ m s}^{-2}.

Graphical Representation of Motion

Graphs are a powerful tool for visualizing and understanding motion.

Distance-Time Graphs

In a distance-time graph, time is plotted on the x-axis and distance on the y-axis.

  • Uniform Speed: The graph is a straight line. The steepness (slope) of the line indicates the speed. A steeper line means a higher speed. The speed can be calculated from the slope: v=s2s1t2t1v = \frac{s_2 - s_1}{t_2 - t_1}
  • Non-uniform Speed: The graph is a curved line. This indicates that the object is accelerating.
  • Object at Rest: The graph is a straight line parallel to the time axis, as the distance does not change.

Velocity-Time Graphs

In a velocity-time graph, time is plotted on the x-axis and velocity on the y-axis.

  • Uniform Velocity (Constant Velocity): The graph is a straight line parallel to the time axis.
  • Uniform Acceleration: The graph is a straight line with a constant slope.
  • Non-uniform Acceleration: The graph can be any curved shape.
Note
The area under a velocity-time graph represents the magnitude of the displacement (or distance travelled) by the object during that time interval. For a rectangle (uniform velocity), the area is velocity × time. For a triangle (uniform acceleration from rest), the area is 12×base×height\frac{1}{2} \times \text{base} \times \text{height}.

Equations of Motion

For an object moving along a straight line with uniform acceleration, we can use a set of three equations to relate its velocity, acceleration, distance, and time. These are known as the equations of motion.

  1. Velocity-Time Relation: v=u+atv = u + at
  2. Position-Time Relation: s=ut+12at2s = ut + \frac{1}{2}at^2
  3. Position-Velocity Relation: 2as=v2u22as = v^2 - u^2

Where:

  • uu = initial velocity
  • vv = final velocity
  • aa = uniform acceleration
  • tt = time
  • ss = distance travelled
Example
Example A train starting from rest attains a velocity of 72 km h172 \text{ km h}^{-1} in 5 minutes. Assuming that the acceleration is uniform, find (i) the acceleration and (ii) the distance travelled by the train for attaining this velocity.

Given

  • Initial velocity, u=0u = 0 (starts from rest)
  • Final velocity, v=72 km h1=20 m s1v = 72 \text{ km h}^{-1} = 20 \text{ m s}^{-1}
  • Time, t=5 minutes=300 st = 5 \text{ minutes} = 300 \text{ s}

To Find

(i) The acceleration, aa (ii) The distance travelled, ss

Formula

a=vuta = \frac{v-u}{t} 2as=v2u22as = v^2 - u^2

Solution

(i) Calculate the acceleration a=20 m s10 m s1300 s=20300 m s2=115 m s2a = \frac{20 \text{ m s}^{-1} - 0 \text{ m s}^{-1}}{300 \text{ s}} = \frac{20}{300} \text{ m s}^{-2} = \frac{1}{15} \text{ m s}^{-2} Answer for part (i) = 115 m s2\frac{1}{15} \text{ m s}^{-2}


(ii) Calculate the distance travelled Using the third equation of motion: 2as=v2u22as = v^2 - u^2 s=v2u22a=(20 m s1)2022×(115) m s2s = \frac{v^2 - u^2}{2a} = \frac{(20 \text{ m s}^{-1})^2 - 0^2}{2 \times (\frac{1}{15}) \text{ m s}^{-2}} s=4002/15 m=400×152 m=3000 m=3 kms = \frac{400}{2/15} \text{ m} = 400 \times \frac{15}{2} \text{ m} = 3000 \text{ m} = 3 \text{ km} Answer for part (ii) = 33 km


Final Answer The acceleration of the train is 115 m s2\frac{1}{15} \text{ m s}^{-2} and the distance travelled is 3 km.

Example
Example A car accelerates uniformly from 18 km h118 \text{ km h}^{-1} to 36 km h136 \text{ km h}^{-1} in 5 s. Calculate (i) the acceleration and (ii) the distance covered by the car in that time.

Given

  • Initial velocity, u=18 km h1=5 m s1u = 18 \text{ km h}^{-1} = 5 \text{ m s}^{-1}
  • Final velocity, v=36 km h1=10 m s1v = 36 \text{ km h}^{-1} = 10 \text{ m s}^{-1}
  • Time, t=5t = 5 s

To Find

(i) The acceleration, aa (ii) The distance covered, ss

Formula

a=vuta = \frac{v-u}{t} s=ut+12at2s = ut + \frac{1}{2}at^2

Solution

(i) Calculate the acceleration a=10 m s15 m s15 s=55 m s2=1 m s2a = \frac{10 \text{ m s}^{-1} - 5 \text{ m s}^{-1}}{5 \text{ s}} = \frac{5}{5} \text{ m s}^{-2} = 1 \text{ m s}^{-2} Answer for part (i) = 1 m s21 \text{ m s}^{-2}


(ii) Calculate the distance covered s=(5 m s1)(5 s)+12(1 m s2)(5 s)2s = (5 \text{ m s}^{-1})(5 \text{ s}) + \frac{1}{2}(1 \text{ m s}^{-2})(5 \text{ s})^2 s=25 m+12(1)(25) ms = 25 \text{ m} + \frac{1}{2}(1)(25) \text{ m} s=25 m+12.5 m=37.5 ms = 25 \text{ m} + 12.5 \text{ m} = 37.5 \text{ m} Answer for part (ii) = 37.537.5 m


Final Answer The acceleration of the car is 1 m s21 \text{ m s}^{-2} and the distance covered is 37.5 m.

Example
Example The brakes applied to a car produce an acceleration of 6 m s26 \text{ m s}^{-2} in the opposite direction to the motion. If the car takes 2 s to stop after the application of brakes, calculate the distance it travels during this time.

Given

  • Acceleration, a=6 m s2a = -6 \text{ m s}^{-2} (opposite direction)
  • Time, t=2t = 2 s
  • Final velocity, v=0 m s1v = 0 \text{ m s}^{-1} (car stops)

To Find

The distance the car travels, ss.

Formula

v=u+atv = u + at s=ut+12at2s = ut + \frac{1}{2}at^2

Solution

First, we need to find the initial velocity (uu) before the brakes were applied. Using the first equation of motion: 0=u+(6 m s2)(2 s)0 = u + (-6 \text{ m s}^{-2})(2 \text{ s}) 0=u12 m s10 = u - 12 \text{ m s}^{-1} u=12 m s1u = 12 \text{ m s}^{-1}

Now, we can calculate the distance travelled using the second equation of motion: s=(12 m s1)(2 s)+12(6 m s2)(2 s)2s = (12 \text{ m s}^{-1})(2 \text{ s}) + \frac{1}{2}(-6 \text{ m s}^{-2})(2 \text{ s})^2 s=24 m+12(6)(4) ms = 24 \text{ m} + \frac{1}{2}(-6)(4) \text{ m} s=24 m12 m=12 ms = 24 \text{ m} - 12 \text{ m} = 12 \text{ m}

Final Answer The car travels 12 m before it stops after the application of brakes.

Uniform Circular Motion

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

An object is accelerating if its velocity is changing. Velocity includes both speed and direction. In uniform circular motion, the speed is constant, but the direction of motion is continuously changing at every point on the circle. Because the velocity is changing, uniform circular motion is an example of accelerated motion.

If an athlete takes tt seconds to go once around a circular path of radius rr, the speed vv is given by the circumference divided by the time: v=2πrtv = \frac{2 \pi r}{t}

Examples of uniform circular motion include:

  • The motion of the Moon and the Earth.
  • An artificial satellite orbiting the Earth.
  • A cyclist on a circular track moving at a constant speed.

Congratulations! You've completed this chapter

Great job reading through all sections. Ready to test your knowledge and reinforce your learning?