Class 11 › Physics › Physics Part I Work, Energy and Power Class 11 Physics · Physics Part I · Chapter 5
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Browse all 60 kits → SummaryThis chapter gives precise physical meanings to work, energy and power, beginning with the scalar (dot) product of vectors, \(\mathbf{A}\cdot\mathbf{B}=AB\cos\theta\). Work done by a constant force is the scalar product of force and displacement, \(W=\mathbf{F}\cdot\mathbf{d}=Fd\cos\theta\), so it can be positive, negative or zero. Kinetic energy is the energy of motion, \(K=\tfrac12 mv^{2}\), and the work-energy theorem states that the net work done on a body equals the change in its kinetic energy. For a variable force, work is the area under the force-displacement graph, found by integration. Potential energy is the energy stored by virtue of position or configuration; gravitational potential energy is \(mgh\) and spring potential energy is \(\tfrac12 kx^{2}\). For conservative forces, the work done is path-independent and total mechanical energy \(K+U\) is conserved. The law of conservation of energy states that energy can be transformed but neither created nor destroyed. Power is the rate of doing work, \(P=\mathrm{d}W/\mathrm{d}t=\mathbf{F}\cdot\mathbf{v}\), with the watt as its SI unit. Collisions are classified as elastic, in which kinetic energy is conserved, and inelastic, in which it is not, while momentum is conserved in both.
The scalar product Notions of work and kinetic energy Work done by a variable force The work-energy theorem Potential energy and conservative forces Conservation of mechanical energy Power Collisions: elastic and inelastic Key termsWork
The product of the component of force along the displacement and the magnitude of displacement, \(W=Fd\cos\theta\).
Kinetic energy
The energy possessed by a body due to its motion, \(K=\tfrac12 mv^{2}\).
Work-energy theorem
The principle that the net work done on a body equals the change in its kinetic energy.
Potential energy
Energy stored in a body by virtue of its position or configuration, such as \(mgh\) or \(\tfrac12 kx^{2}\).
Conservative force
A force for which the work done is independent of the path and depends only on the end points, e.g. gravity.
Power
The time rate of doing work, \(P=\mathrm{d}W/\mathrm{d}t=\mathbf{F}\cdot\mathbf{v}\); SI unit watt.
Extra questions & answersQ1 Define the scalar product of two vectors. Answer Q2 When is the work done by a force zero? Answer Q3 State the work-energy theorem. Answer Q4 How is work done by a variable force calculated? Answer Q5 Write the gravitational and spring potential energies. Answer Q6 What is special about a conservative force? Answer Q7 State the law of conservation of mechanical energy. Answer Q8 Define power and give its SI unit. Answer Q9 Distinguish elastic and inelastic collisions. Answer Q10 What is one electron-volt and one kilowatt-hour? Answer Try one from this chapter
The work done by a constant force is given by:
A \(W=Fd\cos\theta\) B \(W=Fd\sin\theta\) C \(W=Fd\) D \(W=F/d\)
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