Monday, March 12, 2007

Integration

The process of finding integrals is called integration. The process is usually used to find a measure of totality such as area, volume, mass, displacement, etc., when its distribution or rate of change with respect to some other quantity (position, time, etc.) is specified. For example, to find the area between the two curves in the figure, between two limits, would be to evaluate the integral of the function representing the difference in the value of the two functions between those limits.

As an example, if f is the constant function f(x) = 3, then the integral of f between 0 and 10 is the area of the rectangle bounded by the lines x = 0, x = 10, y = 0, and y = 3. The area is the width of the rectangle times its height, so the value of the integral is 30. The same result can be found by integrating the function, though this is usually done for more complicated curves.

The term "integral" may also refer to antiderivatives. Though they are closely related through the fundamental theorem of calculus, the two notions are conceptually distinct. When one wants to clarify this distinction, an antiderivative is referred to as an indefinite integral (a function), while the integrals discussed in this article are termed definite integrals.

The integral of a real-valued function f of one real variable x on the interval [a, b] is equal to the signed area bounded by the lines x = a, x = b, the x-axis, and the curve defined by the graph of f. This is formalized by the simplest definition of the integral, the Riemann definition, which provides a method for calculating this area using the concept of limit by dividing the area into successively thinner rectangular strips and taking the limiting value approached by the sum of their areas as the maximum width of the strips is decreased towards zero (for example see this applet).







Leibniz introduced the standard long s notation for the integral.

Sunday, March 11, 2007

OPTICS AND MODERN PHYSICS

1. LIGHT – RAY OPTICS AND WAVE OPTICS

YEAR

NO.OF Qs

2002

4

2003

3

2004

4

2005

6

2006

1

2. MATTER AND RADIATION

YEAR

NO.OF Qs

2002

2

2003

1

2004

3

2005

3

2006

3

3. ATOMS, MOLECULES AND NUCLEI

YEAR

NO.OF Qs

2002

2

2003

9

2004

3

2005

4

2006

5

SOLIDS AND SEMICONDUCTOR DEVICE

1. CONDUCTORS, SEMICONDUCTORS AND INSULATORS

YEAR

NO.OF Qs

2002

5

2003

3

2004

5

2005

3

2006

6

ELECTROMAGNETISM

1. MAGNETIC EFFECT OF CURRENT AND MAGNETISM

YEAR

NO.OF Qs

2002

6

2003

6

2004

7

2005

7

2006

3

2. ELECTROMAGNETIC INDUCTION & ALTERNATING CURRENT

YEAR

NO.OF Qs

2002

4

2003

4

2004

5

2005

4

2006

5

3. ELECTROMAGNETIC WAVES

YEAR

NO.OF Qs

2002

2

2003

1

2004

1

2005

0

2006

1

OSCILLATIONS

YEAR

NO.OF Qs

2002

3

2003

5

2004

3

2005

2

2006

2

WAVES

YEAR

NO.OF Qs

2002

5

2003

4

2004

3

2005

4

2006

2

ELECTROSTATICS

YEAR

NO.OF Qs

2002

5

2003

5

2004

3

2005

5

2006

3

CURRENT ELECTRICITY

YEAR

NO.OF Qs

2002

1

2003

3

2004

5

2005

3

2006

4

GRAVITATION

YEAR

NO.OF Qs

2002

3

2003

3

2004

4

2005

3

2006

0

PROPERTIES OF MATTER

YEAR

NO. OF Qs

2002

1

2003

0

2004

3

2005

2

2006

HEAT AND THERMODYNAMICS

YEAR

NO. OF Qs

2002

8

2003

7

2004

6

2005

5

2006

3

MECHANICS

1. LAWS OF MOTION

YEAR

NO.OF Qs

2002

3

2003

6

2004

2

2005

7

2006

2

2. WORK, ENERGY AND POWER

YEAR

NO.OF Qs

2002

5

2003

3

2004

4

2005

3

2006

5

3. MOTION OF SYSTEM OF PARTICLES AND RIGID BODY

YEAR

NO.OF Qs

2002

5

2003

3

2004

2

2005

4

2006

4

UNITS AND DIMENSIONS

YEAR

NO.OF Qs

2002

1

2003

2

2004

1

2005

1

2006

1

KINEMATICS

YEAR

NO.O Qs

2002

6

2003

4

2004

8

2005

5

2006

1