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Basic Mathematics for physics, Study notes of Mathematical Physics

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UNIT I
MATHEMATICAL TOOLS
1.1 Basic Mathematics for Physics
Mathematics is the TOOL of Physics. A good knowledge and applications of fundamentals of
mathematics (which are used in physics) helps in understanding the physical phenomena and their
applications. The topics introduced in this chapter enable us to understand topics of first year pre
university physics.
I. Quadratic Equation and its Solution
A second degree equation is called quadratic equation.
The equation, ax2 + bx + c = 0 is a quadratic equation,
In this equation, a, b and c are constants and x is a variable quantity.
The solution of the quadratic equation is
24
2
bb ac
xa
−±
=
Illustration: Comparing the given quadratic equation x2 — 5x + 6 = 0
with the standard form of quadratic equation a x2 +b x + c = 0
We have a = 1, b = -5, c = 6
Now, we know 2
2(5) (5) 416
4
221
bb ac
xx
a
−± ××
−±
=∴=
×
5252451
22
±− ±
==
64
22
32
xor
xorx
=
==
Exercise 1.1:
Solve for x comparing with the standard equation
1. x2 9x + 14 = 0
2. 2x2 + 5x – 12 = 0
3. 3x2 + 8x + 5 = 0
4. 4x2 – 4ax + (a2 – b2) = 0
II. Binomial Theorem
According to this theorem, 23
(1) (2)
(1 ) 1 .......
2! 3!
nnn nn
xnx x x
+=++ + +
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff

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UNIT I

MATHEMATICAL TOOLS

1.1 Basic Mathematics for Physics

Mathematics is the TOOL of Physics. A good knowledge and applications of fundamentals of

mathematics (which are used in physics) helps in understanding the physical phenomena and their

applications. The topics introduced in this chapter enable us to understand topics of first year pre

university physics.

I. Quadratic Equation and its Solution

A second degree equation is called quadratic equation.

The equation, ax

2

  • bx + c = 0 is a quadratic equation,

In this equation, a, b and c are constants and x is a variable quantity.

The solution of the quadratic equation is

2 4

b b ac x a

Illustration: Comparing the given quadratic equation x

2 — 5x + 6 = 0

with the standard form of quadratic equation a x

2 +b x + c = 0

We have a = 1, b = -5, c = 6

Now, we know

2 2 4 ( 5)^ ( 5)^4 1

b b ac x x a

− ± −^ −^ −^ ±^ −^ −^ × ×

×

x or

x or x

Exercise 1.1:

Solve for x comparing with the standard equation

1. x

2 − 9x + 14 = 0

2. 2 x

2

  • 5 x – 12 = 0
  1. 3 x

2

  • 8x + 5 = 0
  1. 4 x

2

  • 4 ax + (a

2

  • b

2 ) = 0

II. Binomial Theorem

According to this theorem,

n n n^ n n x nx x x

Where | x \ < 1, n is any negative integer or any fraction (positive or negative)

The total number of terms = n + 1 i.e. one more than the index of the power of the Binomial.

2! = 2 x 1, 3! = 3 x 2 x 1 and n! = n (n – 1) (n – 2) ( n – 3)..........

If |x| < <1, then the terms containing higher power of x can be neglected.

Therefore (1+ x )

n = 1 + nx****.

Binomial theorem for positive integral index

1 1 ( 1) 2 ( ) ..... 1! 2!

n n n n nx^ a^ n n^ x n x a x a a

− − −

  • = + + + +

where n is any positive integer.

Example 1: Expand (1+x)

-

Solution: (1+x)

-2 ( 2)( 2^ 1)^2 ( 2)( 2^ 1)( 2^ 2) 3

x x x

= − x + xx +

2 3 = 1 − 2 x + 3 x − 4 x +.....

Example 2: Evaluate 37 correct up to three decimal places.

Solution:

1/ 1/2 1/2 1 1/ 37 (36 1) (36) 1 5(1 0.028) 36

2 3

⎜ −^ ⎟ ⎜ −^ ⎟⎜ − ⎟

We have neglected the terms containing powers of 0.028.

∴ 37 = 6 1[ +0.014]

6 1 [ 0.014] 6 1.014[ ]

Exercise:

1. The value of acceleration due to gravity (g) at a height h above the surface of earth is

2

2 ( )

gR g R h

If h<<R, then prove that g’ =

1 - 2h g R

Example: Expand the following using logarithm formulae

(i)

T

f l m

Solution:

1/ 1

T

f l m

Taking log both sides, we get

log f = log T

1/ − log m

1/ − (log 2 + log l )

log log (log 2 log ) (log log ) log 2 log. 2 2 2

= Tm − + l = Tm − − l

Exercise

Expand the following by using logarithm formulae

(i) PV K

γ

= (ii)

l

V

Pr

4

= (iii) rpg

T

h

= (iv) (^2)

l T g

= π

IV. Trigonometry

Angle: Consider a fixed straight line OX. Let another straight line OA (called revolving line) be

coinciding with OX rotate anticlockwise and takes the position OA, The angle is measured by the

amount of revolution that the revolving line OA undergoes in passing from its initial position to final

position_._

From Figure given below, angle covered by revolving line OA is

θ = ∠AOX.

An angle ∠AOX is +ve, if it is traced out in anticlockwise direction and ∠AOX is –ve, if it is

traced out in clockwise direction

A

θ

(^0) X

System of Measurement of an Angle

(i) Sexagesimal System (ii) circular system

(i) Sexagesimal System:

In this system

1 right angle = 90

O (degrees)

1 degree = 60

’ (minutes)

1 minute = 60

’’ (seconds)

(ii) In circular system :

π Radians = 180

O = 2 right angles

1right. Angle = 2

π radians.

Let a particle moves from initial position A to the final position B along a circle of radius r as shown in

figure.

Then, Angle, θ = Radiusof circle ( r )

LenghtofarcAB

If length of arc AB = radius of the circle ( r )

Then θ = 1 radian

Radian: An angle subtended at the centre of a circle by an arc whose length is equal to the

radius of the circle is called one radian.

Relation between Radian and Degree

When a body or a particle completes one rotation, then θ = 360° and distance travelled

(circumference of a circle).

θ = r

2 π r

Or 360

O = 2π radian

Or 1 rad =

O

π

= ×

Thus, 1 radian = 57.

O

B

A

θ

Important relations:

  1. cosec θ =

sin θ

  1. sec θ =

cos θ

  1. cot θ =

tan θ

  1. sin

2 θ+cos

2 θ = 1 5. sec

2 θ = 1 + tan

2 θ 6. cosec

2 θ = 1 + cot

2 θ

Signs of trigonometric ratios

The signs of various trigonometric ratios can be remembered from the above figure.

Trigonometric Ratios of Standard angles

The trigonometric ratios of standard angles are given in the following table:

Angle θ →

trig-ratio

O 30

O 45

O 60

O 90

O 120

O 180

O

sin θ 0

cos θ 1

tan θ 0

Trigonometrical Ratios of Allied Angles

  1. (i) sin (−θ) = − sin θ (ii) cos (−θ) = cos θ (iii) tan (−θ) = − tan θ
  2. (i) sin (

O −θ) = cos θ (ii) cos (

O −θ) = sin θ (iii) tan (

O −θ) = cot θ

  1. (i) sin (

O +θ) = cos θ (ii) cos (

O +θ) = sin θ (iii) tan (

O +θ) = −cot θ

  1. (i) sin (

O −θ) = sin θ (ii) cos (

O −θ) = − cos θ (iii) tan (

O −θ) = − tan θ

  1. (i) sin (

O +θ) = −sin θ (ii) cos (

O +θ) = − cos θ (iii) tan (

O +θ) = − tan θ

  1. (i) sin (

O −θ) = − cos θ (ii) cos (

O −θ) = −sin θ (iii) tan (

O −θ) = cot θ

  1. (i) sin (

O +θ) = −cos θ (ii) cos (

O +θ) = sin θ (iii) tan (

O +θ) = −cot θ

Illustrations:

Find the values of

(i) sin 270

O (ii) sin 120

O (iii) sin 120

O (iv) tan (-

O )

Solution:

(i) sin 270

O = sin (

O

  • 90

O ) = − sin 90

O = − 1

(ii) cos 120

O = cos (

O

  • 30

O ) = − sin 30

O = − 2

(iii) sin 120

O = sin (

O

  • 30

O ) = cos 30

O

2

(iv) tan (− 30

O ) = − tan 30

O = − 3

Some important Trigonometric Formulae

  1. sin (A+B) = sin A cos B + cos A sin B 2. cos (A+B) = cos A cos B − sin A sin B
  2. sin (A−B) = sin A cos B − cos A sin B 4. cos (A−B) = cos A cos B + sin A sin B
  3. sin 2 A = 2 sin A cos A 6. sin (A+B) sin (A−B) = sin

2 A − sin

2 B

  1. cos (A+B) cos (A−B) = cos

2 A − sin

2 B 8. tan (A+B) = A B

A B

1 tan tan

tan tan

  1. sin A + sin B = 2 sin

2

cos 2

A + B A − B

  1. sin A−sin B=2 cos 2

A + B

sin 2

A − B

  1. cos A + cos B = 2 cos

2

A + B

cos 2

A − B

  1. cos A-cos B=−2 sin 2

A + B

sin 2

A − B

  1. If y = Cu , where u is the function of x and C is constant

dx

du C dx

dy

4. If y = u ± v ± ω ± ……, where u, v and ω are the function of x

dx

d v dx

d u dx

d

dx

dy

  1. If y = u v , where u and v are the function of x , then

dx

du

dx

dv u dx

dy = +

  1. If y =

u

v , where u and v are the function of x , then 2 u

dx

du v dx

dv u

dx

dy

  1. If y = u

n , where u is the function of x then dx

du nu dx

dy (^) n − 1

Exercise 1.

1, Find derivative of the functions w.r.t x

(i) 4x

3 +7x

2 +6x+9 (ii) 2

5 5

(^2) x

x(iii)^ x

(iv)

x + 4

Differential coefficients of Trigonometric Functions

d

dx

(sin x ) = cos x ; and

d

dx

(sin u ) = cos u

d u ( )

dx

, u is the function of x

d

dx

(cos x ) = − six x ;

d

dx

(cos u ) = − sin u ( )

d u dx

d

dx

(tan x ) = sec

2 x ;

d

dx

(tan u ) = sec

2 u

d

dx

( u )

d

dx

(cot x ) = − cosec

2 x

d

dx

(sec x ) = sec x tan x

d

dx

(cosec x ) = − cosec x cot x.

Example:

Differentiate the following w.r.t. x****.

(i) sin 2 x (ii) x sin x

Solution:

(i) Let y = sin 2 x

∴ (sin 2 ) cos 2 (2 ) cos 2 .2 2 cos 2

dy d d x x x x x dx dx dx

(ii) Let y = x sin x

∴ ( sin ) (sin ) sin ( ) cos sin.

dy d d d x x x x x x x x x dx dx dx dx

∴ cos sin

dy x x x dx

Exercise 1.

(i) sin 3 x (ii) cos 3 x

(iii) tan 4 x (iv) sin ( ax + b )

(v) cos (ax + b)

Differential Coefficients of Logarithmic and Exponential Functions

(log (^) e ) log e

d x e dx x x

= = ( (Q log e e =1) 2.

(log (^) e ) ( )

d d u u dx u dx

d (^) u u d e e u dx dx

= 4. ( ) log

x x x e

d e e e e dx

d (^) u u d e e u dx dx

Example:

1. Differentiate the follow w.r.t .x.

(i)

2 (log (^) e x ) (ii) log( ax + b )

Solution:

(i) Let y =

2 (log (^) e x )

(log ) 2 log (log ) 2 log. log

dy d d x x x x x dx dx dx x x

(ii) Let y = log( ax + b )

log( ) ( ) ( )

dy d d a ax b ax b dx dx ax b dx ax b

Example 3: If

3 2

S = 2 t − 3 t + 2, find the position, velocity and acceleration of a particle at the end of

2s. S is measured in metre and t in second.

Fundamental Formulae of Integration

dx = x ⎥ ⎦

( x )= 1 dx

d Q 2.

1

n

x x dx

n n provided n ≠ − 1.

dx x x

x dx log e

x x e dx e

ax ax ax e^ e e dx d (^) a ax dx

a

a a dx

e

x x

log

sin xdx = −cos x 7a.

a

ax

ax dx

d

ax axdx

cos

cos sin

cos xdx = sin x 8a.

a

ax axdx

sin cos

sec xdx = tan x

2

cos ec xdx = −cot x

2

sec x tan xdx = sec x 12.

cos ecx cot xdx = −cos ecx

= =− dx x x

x dx x

x x dx log e cos cos

sin

cos

sin tan

= = x

x

xdx

x dx log e sin

sin

cos

cot

− sin ;| | 1

1

1

2

x x

x

dx

  1. sec | |;| | 1

1

1

2

x x

x x

dx

x

x

dx 1

2

tan

Theorems of Integration

First Theorem: The integral of the product of a constant and a function is equal to the product

of the constant and integral of the function.

i. e. cudx = c udx , where c is constant.

Second Theorem: The integral of the sum or difference of a number of functions is given by

( u ± v ±ω±........) dx = udx ± vdx ± ω dx ±.........

Exercise 1.

Integrate the following functions w.r.t .x,

(i) x

3 (ii) x

x

  • (iii) e

3x (iv)

2 1 ⎟ ⎠

x

x (v) x

(vi) 4e

5x

Definite integral

If

F ( ) x dx = f ( ) x + c

Then ( ) ( ) ( )

b

a

F x dx = f bf a

Where a and b are called the upper and lower limits of x

Definite integral is illustrated with the following examples.

Exercise 1.

Solve the following:

(i)

=

=∞

x R

x

dx x

GMm

2

(ii)

/ 2

0

cos

π

x dx (iii)

2

1

3 x dx

(iv)

v

u

m v d v

(v)

/ 2

/ 2

sin

π

π

xd x

Exercise 1.

Solve the following:

(i)

/ 2

/ 2

cos

π

π

x dx (ii)

0

Q q dq C

where C is a constant

(iii)

θ

θ

1

d

where, θ 0 is a constant

(ii)

/ /.

0 cos^ [sin^ ]^0 sin^ sin 0^1 2

x dx x

π

π ⎡^ π ⎤

(iii)

(^2 4 24 ) 3

(^1 )

x x dx

(iv)

2 2 2

2 2

v v^ v

u u (^) u

v v u m v d v m v d v m m

m v u

(v) cos( / 2 ) 0

2

sin [cos ] cos

/ 2

/ 2

/ 2 / (^2) ⎥= ⎦

− π

π

π

π

π xdx x π

Exercise 1.

(i) 2 (ii)

2

Q

C

(iii)

1 0

2 0 log