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Work ,Energy and Power
(1) Introduction
- In our everyday life we use terms like work and enegy.
- Term work is generally used in context to any kind of activity requiring physical or mental effort.
- But this is not the way how we define work done in physics.
- When we push or pull a heavy load or lift it above the floor then we are doing work, but a man carrying heavy load and standing still is not doing any work according to scientific definiton of work.
- Another term we often use is energy. Energy is usually associated with work done in the sence that a person feeling very energetic is capable of doing lot of work.
- This way energy defined to be as capacity of doing work.
- There are many forms of energy like chemical energy, mechanical energy, electrical energy, heat energy etc. These forms of energies can be used in number of ways.
- One form of energy can be converted into another form of energy.
- In this chapter we will study about work, relation between work and energy, conservation of energy etc.
(2) Work
- We already know that work is said to be done when a force produces motion.
- Work done is defined in such a way that it involves both force applied on the body and the displacement of the body.
- Consider a block placed on a frictionless horizontal floor. This block is acted upon by a constant force F. Action of this force is to move the body through a distance d in a straight line in the direction of force.
- Now , work done by this force is equal to the product of the magnitude of applied force and the distance through which the body moves. Mathematically,
W=Fd (1)
where, F=|F|
- Consider the figure given below
- In this case force acting on the block is constant but the direction of force and direction of displacement caused by this force is different. Here force F acts at an angle θ to the displacement d
- Effective component of force along the direction of displacement is Fcosθ and this component of force is responsible for the displacement of the block in the given direction.
- Thus , work done by the force F in in displacing the body thruugh displacement d is
W=(|F|cosθ)|d| (2)
In equation 2 work done is defined as the product of magnitude of displacement d and the component of force in the direction of displacement.
- We know that the scalar product of two vectors A and B where A makes an angle θ with B is given by
A.B=|A| |B|cosθ
- Comparing equation 2 with definition of scalar products work done can be written as
W=F.d (3)
- Now consider two special cases:-
(i) When angle θ=0 i.e., force is in the same direction as of displacement, then from equation (2)
W=|F| |d|
this is the same result as of equation 1
(ii) when angle θ=90 i.e., direction of force is perpandicular to that of displacement, then from equation (2)
W=(|F|cos90)|d|=0
that is force applies has no component along the displacement and hence force does not do any work on the body.
- Work done by a force on a body can be positive, negative and zero i.e.,
(a) Work done is positive :- Force is in the same direction as displacement for example work done by force for pushing a block of mass m
(b) Work done is negative :- Force is opposite to the displacement for example when a body slides on horisontal surface work done by frictional forces on body is negative as frictional force always acts opposite to displacement of the body.
(c) Work done is zero :- Force is at rigt angle to the displacement for example work of a centripetal force on a body moving in a circle.
- Unit of work done in any system of units is equal to the unit of force multiplied by the unit of distance. In SI system unit of work is 1Nm and is given a name Joule(J). Thus,
1J=1Nm
In CGS system unit is erg
1erg=1 dyne-cm
and 1 erg=10-7J
- When more then one forces acts on a body then work done by each force should be calculated separately and added togather.
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