
1.Basic Maths (1) : Vectors
7
Lecture1.1

Lecture1.2

Lecture1.3

Lecture1.4

Lecture1.5

Lecture1.6

Lecture1.7


2.Basic Maths (2) : Calculus
4
Lecture2.1

Lecture2.2

Lecture2.3

Lecture2.4


3.Unit and Measurement
13
Lecture3.1

Lecture3.2

Lecture3.3

Lecture3.4

Lecture3.5

Lecture3.6

Lecture3.7

Lecture3.8

Lecture3.9

Lecture3.10

Lecture3.11

Lecture3.12

Lecture3.13


4.Motion (1) : Straight Line Motion
10
Lecture4.1

Lecture4.2

Lecture4.3

Lecture4.4

Lecture4.5

Lecture4.6

Lecture4.7

Lecture4.8

Lecture4.9

Lecture4.10


5.Motion (2) : Graphs
3
Lecture5.1

Lecture5.2

Lecture5.3


6.Motion (3) : Two Dimensional Motion
6
Lecture6.1

Lecture6.2

Lecture6.3

Lecture6.4

Lecture6.5

Lecture6.6


7.Motion (4) : Relative Motion
7
Lecture7.1

Lecture7.2

Lecture7.3

Lecture7.4

Lecture7.5

Lecture7.6

Lecture7.7


8.Newton's Laws of Motion
8
Lecture8.1

Lecture8.2

Lecture8.3

Lecture8.4

Lecture8.5

Lecture8.6

Lecture8.7

Lecture8.8


9.Constrain Motion
3
Lecture9.1

Lecture9.2

Lecture9.3


10.Friction
6
Lecture10.1

Lecture10.2

Lecture10.3

Lecture10.4

Lecture10.5

Lecture10.6


11.Circular Motion
6
Lecture11.1

Lecture11.2

Lecture11.3

Lecture11.4

Lecture11.5

Lecture11.6


12.Work Energy Power
12
Lecture12.1

Lecture12.2

Lecture12.3

Lecture12.4

Lecture12.5

Lecture12.6

Lecture12.7

Lecture12.8

Lecture12.9

Lecture12.10

Lecture12.11

Lecture12.12


13.Momentum
9
Lecture13.1

Lecture13.2

Lecture13.3

Lecture13.4

Lecture13.5

Lecture13.6

Lecture13.7

Lecture13.8

Lecture13.9


14.Center of Mass
5
Lecture14.1

Lecture14.2

Lecture14.3

Lecture14.4

Lecture14.5


15.Rotational Motion
14
Lecture15.1

Lecture15.2

Lecture15.3

Lecture15.4

Lecture15.5

Lecture15.6

Lecture15.7

Lecture15.8

Lecture15.9

Lecture15.10

Lecture15.11

Lecture15.12

Lecture15.13

Lecture15.14


16.Rolling Motion
11
Lecture16.1

Lecture16.2

Lecture16.3

Lecture16.4

Lecture16.5

Lecture16.6

Lecture16.7

Lecture16.8

Lecture16.9

Lecture16.10

Lecture16.11


17.Gravitation
8
Lecture17.1

Lecture17.2

Lecture17.3

Lecture17.4

Lecture17.5

Lecture17.6

Lecture17.7

Lecture17.8


18.Simple Harmonic Motion
13
Lecture18.1

Lecture18.2

Lecture18.3

Lecture18.4

Lecture18.5

Lecture18.6

Lecture18.7

Lecture18.8

Lecture18.9

Lecture18.10

Lecture18.11

Lecture18.12

Lecture18.13


19.Waves (Part1)
11
Lecture19.1

Lecture19.2

Lecture19.3

Lecture19.4

Lecture19.5

Lecture19.6

Lecture19.7

Lecture19.8

Lecture19.9

Lecture19.10

Lecture19.11


20.Waves (Part2)
10
Lecture20.1

Lecture20.2

Lecture20.3

Lecture20.4

Lecture20.5

Lecture20.6

Lecture20.7

Lecture20.8

Lecture20.9

Lecture20.10


21.Mechanical Properties of Solids
6
Lecture21.1

Lecture21.2

Lecture21.3

Lecture21.4

Lecture21.5

Lecture21.6


22.Thermal Expansion
5
Lecture22.1

Lecture22.2

Lecture22.3

Lecture22.4

Lecture22.5


23.Heat and Calorimetry
2 
24.Heat Transfer
6
Lecture24.1

Lecture24.2

Lecture24.3

Lecture24.4

Lecture24.5

Lecture24.6


25.Kinetic Theory of Gases
6
Lecture25.1

Lecture25.2

Lecture25.3

Lecture25.4

Lecture25.5

Lecture25.6


26.Thermodynamics
9
Lecture26.1

Lecture26.2

Lecture26.3

Lecture26.4

Lecture26.5

Lecture26.6

Lecture26.7

Lecture26.8

Lecture26.9


27.Fluids
14
Lecture27.1

Lecture27.2

Lecture27.3

Lecture27.4

Lecture27.5

Lecture27.6

Lecture27.7

Lecture27.8

Lecture27.9

Lecture27.10

Lecture27.11

Lecture27.12

Lecture27.13

Lecture27.14


28.Surface Tension and Viscosity
6
Lecture28.1

Lecture28.2

Lecture28.3

Lecture28.4

Lecture28.5

Lecture28.6

Chapter Notes – Work Energy Power
WORK
Whenever a force acting on a body produces a change in the position of the body, work is said to be done by the force. If there is no change in the position of the body, work is not done. Our special definition of the word work does not correspond to the colloquial usage of the term. Thus, we may exert a large force on a wall, but if the wall remains where it is, then we have not done any work. We may be doing hard work in physiological sense, but from the point of view of physics, we are not doing any work. If a coolie holding a heavy box on his head is standing at a fixed location, he is not doing any work. Work is said to be done only when there is a displacement in the direction of force.
The work W done by a constant force F when its point of application undergoes a displacement s is defined to be
W=Fscosθ
where θ is the angle between F⃗ and s⃗ as indicated in figure. Only the component of F⃗ along s, that is fcosθ, contributes to the work done. Strictly speaking, the work is done by the source or agent that applies the force. Work is a scalar quantity and its SI unit is the joule (J). From the above equation, we see that
1 J = 1 Nm
Work is also defined as the dot product of force and its displacement as given by
W=F⃗ .s⃗
In terms of rectangular components, the two vectors are F⃗ =Fxi^+Fyj^+Fzk^ and
s⃗ =Δxi^+Δyj^+Δzk^; hence, the above equation may be written as
W=FxΔx+FyΔy+FzΔz
The work done by a given force on a body depends only on the force, the displacement, and the angle between them. It does not depend on the velocity or the acceleration of the body, or on the presence of other forces.
When several forces act on a body one may calculate the work done by each force individually. The net work done on the body is the algebraic sum of individual contributions.
Wnet=F⃗ 1.S⃗ 1+F⃗ 2.S⃗ 2+……….+F⃗ n.S⃗ n
or W_{net} = W_{1} + W_{2 } + …………… + W_{n}
Positive, Negative and Zero Work
Work done by a force may be positive or negative depending on the angle θ between the force and displacement. If the angle θ is acute (θ < 90^{o}), then the work done is positive and the component of force is parallel to the displacement.
If the angle θ is obtuse (θ > 90^{o}), the component of force is antiparallel to the displacement and the work done by force is negative.
Application 1
When a person lifts a body from the ground to some higher position, the work done by the lifting force (i.e. the force applied by the person ) is positive since force (vector) and displacement (vector) are along the same (vertically upward) direction and hence,
θ=0 cosθ=1
However, the work done by the gravity (or the force by the earth on the body) is negative since force (vector) and displacement (vector) are oppositely directed and hence θ=180^{0 } cosθ=−1.
Application 2
A box is moved over a horizontal path by applying force F = 60 N at an angle = 30^{o} to the horizontal. What is the work done during the displacement of the box over a distance of 0.5 km.
Solution
By definition, W = F s cosθ
Here F = 60 N; s = 0.5 km = 500m; θ = 30^{o
}W = (60)(500) cos30^{o} = 26 kJ
Work Done By Friction
There is a misconception that the force of friction always does negative work. In reality, the work done by friction may be zero, positive or negative depending upon the situation.
In figure (a), when a block is pulled by a force F and the block does not move, the work done by friction is zero.
In figure (b), when a block is pulled by a force F on a stationary surface, the work done by the kinetic friction is negative.
In figure (c), block A is placed on the block B. When the block A is pulled with a force F, the friction force does negative work on block A and positive work on block B. The kinetic friction and displacement are oppositely directed in case of block A while in case of block B they are in the same direction.
Work Done By Gravity
Consider a block of mass m which slides down a smooth inclined plane of angle θ.
Let us assume the coordinate axes as shown in the figure, to specify the components of the two vectors – although the value of work will not depend on the orientation of the axes.
Now, the force of gravity, F⃗ g=−mgj^ and the displacement is given by
S⃗ =Δxi^+Δyj^+Δzk^
The work done by gravity is
Wg=F⃗ g.s⃗ =−mgj^.(Δxi^+Δyj^+Δzk^)
or Wg=−mgΔy (j^.i^=0, j^.i^=1, j^.k^=0)
since Δy = y_{f} – y_{i} = –h
W_{g} = mg(y_{f} – y_{i}) = +mgh
If the block moves in the upward direction, then the work done by gravity is negative and is given by
W_{g} = mgh
NOTE
The work done by the force of gravity on a particle depends only on the initial and final vertical coordinates. It does not depend on the path taken or on the speed of the particle.
The work done by gravity is zero for any path that returns to its initial point.
Application 3
A block of mass 10 kg is to be raised from the bottom to the top of incline 5m long and 3m off the ground at the top. Assuming frictionless surface, how much work is done by a force parallel to the incline pushing the block up at constant speed. ( g = 10 m/s^{2})
Solution
Here, we must first find the force with which the block must be pushed. We begin by drawing a F.B.D. of the block.
Here,
F = Applied force
mg = weight of the block
N = Normal reaction by the incline on the block.
Because the motion occurs at constant speed (i.e. no acceleration), the resultant force parallel to the plane must be zero. Thus
F−mgsinθ=0
or F=mgsinθ=10×1035=60N
Then, the work done by F is
W = F. S cos 0^{0} = 60 × 5 = 300 J.
If a person were to raise the block vertically without using the incline, the work he would do would be the vertical force mg times the vertical distance
or (10 10 N) × (3m) = 300 J, the same as before.
The only difference is that with the incline he could do the job with a smaller force i.e. 60 N but he has to push the block a greater distance i.e. 5 m up the incline than he had to raise the block directly (3m).
This application also illustrates the point that machines (simple or complex) can not save the amount of work that has to be done to accomplish a job, they merely allow us to do the job with less effort.
Work Done By A Variable Force
When the magnitude and direction of a force vary in three dimensions, it can be expressed as a function of the position vector F⃗ (r), or in terms of the coordinates F⃗ (x,y,z). The work done by such a force in an infinitesimal displacement ds is
dW=F⃗ .ds
The work done in going from point A to point B by this variable force F⃗ as shown in the figure is
WA→B=∫ABF⃗ .ds⃗ =∫AB(Fcosθ)ds
In terms of rectangular components,
F⃗ =Fxi^+Fyj^+Fzk^
and ds⃗ =dxi^+dyj^+dzk^
WA→B=∫xAxBFxdx+∫yAyBFydy+∫zAzBFzdz
Work Done By Spring Force
If x be the displacement of the free end of the spring from its equilibrium position then, the magnitude of spring force is given by
F_{x} = kx.
The negative sign signifies that the force always opposes the extension (x > 0) or the compression (x < 0) of the spring. In other words, the force tends to restore the system to its equilibrium position.
The work done by the spring force for a displacement from x_{i} to x_{f} is given by
Ws=∫xixfFsdx=−∫xixfkxdx
or Ws=−12k(x2f−x2i)
Graphically, the work done by the spring force in a displacement from x_{i} to x_{f} is the shaded area (as shown in the figure, which is the difference in the areas of two triangles.
Note
(1)The work done by a spring force may be positive or negative
(2)The work done by the spring force only depends on the initial and final positions.
(3)The work done by the spring force is zero for any path that returns to the initial position.
When already stretched or compressed spring is allowed to regain its natural length, work done by the spring force is positive.
In general, the work done by a variable force F(x) from an initial point x_{i} to final point x_{f} is given by the area under the force – displacement curve as shown in the figure .
Area (work) above the x – axis is taken as positive, and below xaxis is taken as negative.
Application 4
A horizontal force F very slowly lifts the bob of a simple pendulum from a vertical position to a point at which the string makes an angle q_{o} to the vertical. The magnitude of the force is varied so that the bob is essentially in equilibrium all times. What is the work done by the force on the bob?
Solution
Figure is a free body diagram of the system and shows the forces acting on the bob. Since the acceleration is zero, net horizontal force and net vertical force on the bob must be zero.
∑Fx=F−Tsinθ=0
∑Fy=Tcosθ−mg=0
Eliminating T we get
F=mgtanθ …………(i)
This is how the force must vary as a function of angle q in order for the bob to be in equilibrium.
The work done by in an infinitesimal displacement along the circular arc is
dW=F⃗ .ds⃗ =Fxdx
=mgtanθdx ……..(ii)
From figure, we see that dydx=tanθ, thus, dy = tan dx.
Equation (ii) becomes dW = mg dy, therefore, the total work done from
y = 0 to y = y_{o} is
w=∫0yomgdy=mgyo
where the vertical displacement y_{o} is y_{o} = L(1 – cosθ_{o})
W = mgL(1 – cosθ_{o})
Dependence of Work on Frame of Reference
Work as defined, depends on frame of reference also. When we change from one inertial reference frame to another inertial reference frame, the force does not change, while displacement may change, so the work done by a force will be different. For example, suppose a person is pushing a box in a moving train (in the same direction as the movement of train) by applying a force F on it. In the reference frame of the train, the work done by the force will be F. S where S is the displacement of the block with respect to the train. But in the reference frame of the earth the work will be F. (S + S_{0}) where S_{0} is the displacement of the train with respect to the earth.