It is impossible for a man to learn what he thinks he already knows.

.

Quotes

It is impossible for a man to learn what he thinks he already knows.
Notes

Never stop learning because life never stop Teaching

Never stop learning because life never stop Teaching
Showing posts with label ***Matric & intermediate Notes***. Show all posts
Showing posts with label ***Matric & intermediate Notes***. Show all posts

Sunday, 11 October 2015

Health is blessing

health Is Blessing

Health is wealth. There is nothing in our life that is more important than great health. Without health there is no bliss, no peace and no achievement. A man with terrible health can't appreciate the joy of being affluent.

health is more important than cash. Cash can't purchase health and bliss. Be that as it may, a solid individual stays in a condition of delight and joy.

A sound individual is totally free from any sickness or harm. A man with sound health appreciates a steady health that likewise incorporates a solid mental condition. Our health relies on a few components, for example, nourishment, contamination, resting propensities, mental condition, air, water and daylight. Morning strolls and Physical activities are exceptionally useful for the wellness of our psyche and body. We ought to take legitimate consideration of our health with the goal that we can make the most of our life totally.

When we are sick or we would prefer not to play or work, our awful health denies us of sound rest and craving. Life turns into a weight for one, who is always weak. Life has little appeal for him. He feels tired of life, continually griping around one thing or the other.

Then again, one with great health makes the most of his life. When he lives up to expectations or plays he is never drained. A solid individual appreciates great sustenance and sound rest. For him the world is wonderful and life is all euphoria.

A solid individual sings the eminence of life and strives to understand his fantasies. He never whines. He is constantly glad and bright. He may be poor, he may need to work hard to acquire his living, however even the wealthiest man would begrudge him for his great health.

Friday, 26 December 2014

Good by Mr. Chips Important Questions

Good by Mr. Chips

 Important Questions

Describe Mr. Chips first meeting with Mr. Wetherby?
Describe the tragic death of Katherine?
Describe the tragic seen of Mr. Chips Death?
What was Mr. Chips Will?
Where did Mr. Chips live after his retirement? How Mr. Chips did spend his retired life? Or what were the activities of Mr. Chips after retirement?
How Mr. Chips did meet Katherine for the first time?
What were the views of Chips and Katherine about politics?
Write a note on Brookfield or what kind of school was Brookfield?
What contributions did Brookfield make to England?
Draw a character sketch of Mr. Chips.
Write a note on Mr. Chips as a teacher.
Write an account on Mr. Chips married life.
What influence did Katherine Bridges exercise on Mr. Chips?
Describe the first encounter between Mr. Chips and Katherine bridges?
Describe briefly the quarrel between Mr. Chips and Ralston?
Write a note Mr. Chip’s humor.
Can we look upon Mr. Chips as an institution of Brookfield?
Draw a Character sketch of Katherine Bridges?
Write a note on views and ideas on Katherine bridges?
Write a brief note on Mr. Wetherby.
Write a brief note on Mr. Meldrum.
Write a note on Mr. Ralston.

Write a brief note on Chatteris.
Write a brief note on Mr. Merivale.
Write a note on Mrs. Wickett.
Who was Mr. Collingwood?
Who was Linford?
Who was Cartwright?
What kind of books read by Mr. Chips?
What were the difficulties Chips faced when he tried to write a book on collection of his memories? Or what were the difficulties Chips faced when he tried to write a book on

Brookfield?
What were the two things Mr. Chips never done in his life?
When was the Brookfield established?
When and why Mr. Chips retired?
Why was Mr. Ralston not liked at Brookfield?
How did Mr. Chips entertain new comers?
Describe briefly Mr. Chips Farewell speech.
How did Mr. Chips political views were different from Katherine Bridges?
Who said for the first time “Good Bye” Mr. Chips and when?

Wednesday, 24 December 2014

GOOD BYE MR.CHIPS Notes

GOOD BYE MR.CHIPS Notes

QUESTION 1: Who was wetherby? describe the first meeting between him and Mr. Chips.
Ans: Wetherby was the head of Brookfield school when Mr. Chips joined it in 1870. Wetherby was a very polite and decent fellow. During the first interview he encouraged Mr. Chips

very much. He received him very warmly in his study. He told Mr. Chips that he knew why he left  Melburg school. Wetherby told him that his discipline would improve with the passage

of time, as it was a matter of experience. Mr. Chips did not forget his this meeting with Wetherby. Mr. Chips could not forget the encouragement that was given to him by Wetherby.

QUESTION 2: Who was colley and why did Mr. Chips remembered him?
Ans: Colley was the first student who got punishment from Mr. Chips during his first lecture. He dropped the lid of the desk and Mr. Chips gave him hundred lines to write as punishment.

Then his son and grandson came to Brookfield and they were also taught by Mr. Chips. Mr. Chips used to make fun of all the colleys and considered them all dunces and naughty. He used

to tell colley junior that he was the most stupid of all.  

QUESTION 3: What did Mr. Chips teach at Brookfield and what were his ideas about those subjects?
Ans: Mr. Chips taught Greek and Latin at Brookfield. He loved his subjects. He was of the view of that these languages should have been treated as living as other languages spoken by

people. He felt happy to be associated with these languages and according to him people who understood and used these languages were an honourable community.

QUESTION4: Describe the first meeting of Mr. Chips and Katherine Bridges.
Ans: The first meeting of Mr. Chips and Katherine is the most beautiful and important incident of the novel. Chips were visiting Lake District during his summer vacation. One day he saw

a girl standing on a dangerous rock and waving excitedly. He thought that she needed help. He ran towards her and in doing so he slipped himself and got his ankle wrenched. When he

fell, Katherine rushed to help him. Chips found himself rescued instead of the rescuer. After that incident, Katherine kept on looking after him. Mr. Chips was altogether against the

modern women and the freedom she liked. But this charming girl changed his outlook entirely and very soon they fell in love with each other, and got married.  

QUESTION 5: What were the views of Mr. Chips about himself?
Ans: Mr. Chips was a man who loved to live with realities. He never thought high about himself. Most of the time he used to think that he was not capable of doing excellent things. His

degree was mediocre and he would never get promotion. He rated himself as an average teacher. Occasional difficulties in maintaining discipline in classes also troubled him a lot. After

getting married to Katherine he shared his views with her and she used to take all things very lightly and laughed only in reply. However, after his marriage he changed a lot and became

a new man  who was far better than the bachelor chips.


QUESTION 6: How did students of chips behave on the occasion of April fool?
Ans: First April 1898 was the day when his new born baby and wife died . He was very sad and downcast, every thing had lost its charm and attraction and he also wanted to die. On that

very day he received a lot of addressed to him and when he opened them they contained nothing but blank papers. Actually this was April fool and all these letters had been sent to him

by his students. He was so absorbed in his sorrow and preoccupied with his thoughts that he took no notice of it.

QUESTION7:How did Mr. Chips feel after his marriage with Katharine Bridges?
ANS: Mr. Chips was 48 years old and when he married Katherine who was 25 years old. During their short marrital life Chips considered himself to have found all the happiness in this

world he became Questionuite a changed person who was loved honoured and obeyed at Brookfield. Katherine Bridges was a loving wife and s.he made Chips also loving and caring after

his marriage with Katherine. Chips could hardly believe that it could ever have happened before or since in the world. Unfortunately she died in childbirth and chips again remained

alone in this world but still he could remember her and got unlimited inspiration out of the sweet memories of his wife and his married life.

QUESTION8: How did Mr. Chips want to preserve his memories?
ANS: Mr. Chips became Questionuite lonely after the death of his wife and after retirement when he used to sit near the fire at Mr. Wicket innumerable memories thronged his mind. He

used to remember time passed with Katherine and he recollected the names of a lot of boys. He loved his past and its memories so passionately that he wanted to keep them  new and

fresh. Once he decided to write all  his memories and while living at Mr. Wicket’s he started writing desultory notes but writing tired him mentally and physically and he gave it up.

Secondly he felt that all those memories in written form had lost that charm and beauty which they used to have while staying in his mind. However he had a firm resolve to arrange all

those memories in written form.

QUESTION9:When did Mr. Chips became head of Brookfield and was he successful in doing his duties?
ANS: In 1900 old Meldrum, who  succeeded Wetherby and  remained Head for 30 years, suddenly died. After his death Brook field had to have a new head and it took the  board of

governors some time to appoint the new Head. During this interval Chips became acting head. There was possibility that this would turn into permanent appointment Mr. Chips had no

liking for it and he was absolutely not disappointed when a new Head was appointed. During his short period as Head he performed his duties
Questionnaire up to the mark and efficiently.

QUESTION 10: Influence of Katherine bridges on Mr. Chips regarding disciplinary problems in particular. Discuss?
Ans: Katherine bridge after marriage with Mr. Chips made him Questionuite a changed person. He felt himself more stronger and confident than he used to be before his marriage.

Katherine bridges had conquestionuered him completely and he never kept anything from her He used to discuss with her even the slightest problems. Before his marriage he was hard,

dry and neutral sort of person. After his marriage his discipline became better. Katherine directly took part in the affairs of school. She made him broad minded and students were happy

with him. Whenever he was on the verge of punishing any student she stopped him and asked him to give the boy another chance. She was not in the favour of punishing boys. She

always advised him not to report the cases of boys to Head and he always agreed. She was so influential throughout her life that after her death whenever he was confronted with any
problem. He wished that she were alive to give her valued opinion

Sunday, 7 December 2014

essay - Courtesy

 Courtesy

Courtesy means polite behaviour . It springs from smart breeding and kindness of heart. A courteous man isalways polite and observes manner at all occasions . Healways repects the emotions of others and doesn't hurt them at any price.Courtesy demands that we must always be polite and pleasant inevery field of life. Our faith lays nice stress on the necessity of courtesy.Islam teaches USA politeness and manner in each sphere of life.Muslims greet each other, language "Assalam-u-Alakum", and that they oftenadd some remarks regarding
each other’s health and welfare .Courtesy demands that we must always speak gently to everybody. Our words could break a heart or heal it. Courtesy prices nothing however it pays plenty.It consoles the long-faced souls. It brings us sincere friends.Good manners demand that we must always stay up for our turn. during a crowded bus, we must always offer our seat for the ladies, weak or disabled persons. we must always facilitate the blind to cross the road. we must always respect humanity so as to form lifestyle extremely comfortableand worth living . Courtesy amply fulfils this need.

essay My House

  My House

"East or West, home is the best". It is a famous old proverb  which is true to the hilt . My house is situated onthe main road. It is not far  from my school. It is double storeyed. It isfitted with electricity. There are four rooms in each floor. There are marblechips on the floor. We have covered the drawing room with wall to wallcarpet. The show-cases in the drawing room have been tastefullydecorated. It has a kitchen and a bath. It has four bed rooms. I have afolding study-table in a corner of the drawing room where I study and do myhome-work.
All the rooms of my house are airy, neat and clean. They are white-washed every year. We have all the facilities of modern life in our house.Very nice people live around us.I have grown many beautiful flowers in one corner of my house. Their fragrance refreshes me and my family. I love my house very much. Iam proud of my house. God bless our home.

Saturday, 6 December 2014

Essay--My Hobby

Essay

MY HOBBY:

There are many hobbies like gardening, stamp collecting and reading. According to one’s taste and purse.
Stamp collecting and gardening are my favorite hobbies. I remember my uncle gave me two albums of stamps. From that day, I have been adding to them, now I have five albums of stamp.
I collect stamps from various sources. No doubts, I buy same stamps but most of them are collected by others. My father brings stamps from his office more ever; I have pen-friends and often send stamps to each other’s.
Stamps are of great value. They unfold the whole history of the world. Through stamps we can say that this hobby is very informative. Besides stamp collecting, I have another hobby and it is gardening, through it I become fresh and feel strength in my soul. It is very cheap but useful hobby. I spend fen respect as whole and get fresh vegetables for my kitchen. There is a small plat in my house. There I have grown many flower plants. They are very fragment. They give sweet smell whenever I am free and sit near these plants and enjoy their smell.
“Nature never betrays anyone who loves her”.
Gardening provides me a good exercise. It keeps me healthy fresh and happy for the days labor.
Gardening is my sincere friend. I feel new life in my soul. It is better to spend a busy life because
“An empty mind is devil’s workshop”.
This hobby is very interesting. It gives pleasure fragrance and strength. It also removes sadness of mind. Moreover, hobbies have a very educative value. It gives strength for better living.

Sports and Games

ESSAYS FOR matric STUDENTS


 Sports and Games

Sports and games play a big role within the development of human personality . they're as vital for human body as foodgrains and H2O. They keep us active, healthy and good.Games and sports are referred to as co-curricular activities .They are a very important a part of our school information . Pakistanistudents are very keen on sports and games. The facilities are, of course , inadequate nowadays. things is predicted toimprove in close to future.Games and sports produce in us the sense of discipline . Thecaptain of the team works sort of a General and therefore the team must conform thecaptain. of these things produce sport spirit within the minds and souls of the players. They learn to guide their life during a disciplined manner.Games and sports are a awfully smart and helpful supply of recreation. They utililze the vacant time of the young generation.So their temperament develops and that they don't indulge in suchactivities like gambling and drinking .Sports and games keep our body and soul healthy. A sound mind isalways during a sound body. Health is Wealth. If one loses his health, he willnot be able to perform his duties expeditiously . As a result, he willbe left behind within the race of progress.

My Last day at school

My Last day at school

Wednesday, 24 September 2014

Motion in two Dimension

Motion in two Dimension

Projectile Motion

A body moving horizontally as well as vertically under the action of gravity simultaneously is called a projectile. The motion of projectile is called projectile motion. The path followed by a projectile is called its trajectory.
Examples of projectile motion are
1. Kicked or thrown balls
2. Jumping animals
3. A bomb released from a bomber plane
4. A shell of a gun.

Analysis of Projectile Motion
Let us consider a body of mass m, projected an angle θ with the horizontal with a velocity V0. We made the following three assumptions.
1. The value of g remains constant throughout the motion.
2. The effect of air resistance is negligible.
3. The rotation of earth does not affect the motion.

Horizontal Motion
Acceleration : ax = 0
Velocity : Vx = Vox
Displacement : X = Vox t

Vertical Motion
Acceleration : ay = – g
Velocity : Vy = Voy – gt
Displacement : Y = Voy t – 1/2 gt2

Initial Horizontal Velocity
Vox = Vo cos θ …………………. (1)

Initial Vertical Velocity
Voy = Vo sin θ …………………. (2)
Net force W is acting on the body in downward vertical direction, therefore, vertical velocity continuously changes due to the acceleration g produced by the weight W.
There is no net force acting on the projectile in horizontal direction, therefore, its horizontal velocity remains constant throughout the motion.

X – Component of Velocity at Time t (Vx)
Vx = Vox = Vo cos θ ……………….. (3)

Y – Component of Velocity at Time t (Vy)
Data for vertical motion
Vi = Voy = Vo sin θ
a = ay = – g
t = t
Vf = Vy = ?
Using Vf = Vi + at
Vy = Vo sin θ – gt ……………….. (4)

Range of the Projectile (R)
The total distance covered by the projectile in horizontal direction (X-axis) is called is range
Let T be the time of flight of the projectile.
Therefore,
R = Vox x T ………….. {since S = Vt}
T = 2 (time taken by the projectile to reach the highest point)
T = 2 Vo sin θ / g
Vox = Vo cos θ
Therefore,
R = Vo cos θ x 2 Vo sin θ / g
R = Vo2 (2 sin θ cos θ) / g
R = Vo2 sin 2 θ / g ……………… { since 2 sin θ cos θ = sin2 θ}
Thus the range of the projectile depends on
(a) The square of the initial velocity
(b) Sine of twice the projection angle θ.

The Maximum Range
For a given value of Vo, range will be maximum when sin2 θ in R = Vo2 sin2 θ / g has maximum value. Since
0 ≤ sin2 θ ≤ 1
Hence maximum value of sin2 θ is 1.
Sin2 θ = 1
2θ = sin(-1) (1)
2θ = 90º
θ = 45º
Therefore,
R(max) = Vo2 / g ; at θ = 45º
Hence the projectile must be launched at an angle of 45º with the horizontal to attain maximum range.

Projectile Trajectory
The path followed by a projectile is referred as its trajectory.
We known that
S = Vit + 1/2 at2
For vertical motion
S = Y
a = – g
Vi = Voy = Vo sin θ
Therefore,
Y = Vo sinθ t – 1/2 g t2 ………………….. (1)
Also
X = Vox t
X = Vo cosθ t ………… { since Vox = Vo cosθ}
t = X / Vo cos θ

(1) => Y = Vo sinθ (X / Vo cos θ) – 1/2 g (X / Vo cos θ)2
Y = X tan θ – gX2 / 2Vo2 cos2 θ
For a given value of Vo and θ, the quantities tanθ, cosθ, and g are constant, therefore, put
a = tan θ
b = g / Vo2 cos2θ
Therefore
Y = a X – 1/2 b X2
Which shows that trajectory is parabola.

Uniform Circular Motion

If an object moves along a circular path with uniform speed then its motion is said to be uniform circular motion.

Recitilinear Motion
Displacement → R
Velocity → V
Acceleration → a

Circular Motion
Angular Displacement → θ
Angular Velocity → ω
Angular Acceleration → α

Angular Displacement
The angle through which a body moves, while moving along a circular path is called its angular displacement.
The angular displacement is measured in degrees, revolutions and most commonly in radian.
Diagram Coming Soon
s = arc length
r = radius of the circular path
θ = amgular displacement

It is obvious,
s ∞ θ
s = r θ
θ = s / r = arc length / radius

Radian
It is the angle subtended at the centre of a circle by an arc equal in length to its radius.
Therefore,
When s = r
θ = 1 radian = 57.3º

Angular Velocity
When a body is moving along a circular path, then the angle traversed by it in a unit time is called its angular velocity.
Diagram Coming Soon
Suppose a particle P is moving anticlockwise in a circle of radius r, then its angular displacement at P(t1) is θ1 at time t1 and at P(t2) is θ2 at time t2.
Average angular velocity = change in angular displacement / time interval
Change in angular displacement = θ2 – θ1 = Δθ
Time interval = t2 – t1 = Δt
Therefore,
ω = Δθ / Δt
Angular velocity is usually measured in rad/sec.
Angular velocity is a vector quantity. Its direction can be determined by using right hand rule according to which if the axis of rotation is grasped in right hand with fingers curled in the direction of rotation then the thumb indicates the direction of angular velocity.

Angular Acceleration
It is defined as the rate of change of angular velocity with respect to time.
Thus, if ω1 and ω2 be the initial and final angular velocity of a rotating body, then average angular acceleration “αav” is defined as
αav = (ω2 – ω1) / (t2 – t1) = Δω / Δt
The units of angular acceleration are degrees/sec2, and radian/sec2.
Instantaneous angular acceleration at any instant for a rotating body is given by
Angular acceleration is a vector quantity. When ω is increasing, α has same direction as ω. When ω is decreasing, α has direction opposite to ω.

Relation Between Linear Velocity And Angular Velocity
Consider a particle P in an object in X-Y plane rotating along a circular path of radius r about an axis through O, perpendicular to the plane of figure as shown here (z-axis).
If the particle P rotates through an angle Δθ in time Δt,
Then according to the definition of angular displacement.
Δθ = Δs / r
Dividing both sides by Δt,
Δθ / Δt = (Δs / Δt) (1/r)
=> Δs / Δt = r Δθ / Δt
For a very small interval of time
Δt → 0

Alternate Method
We know that for linear motion
S = v t ………….. (1)
And for angular motion
S = r θ …………….. (2)
Comparing (1) & (2), we get
V t = r θ
v = r θ/t
V = r ω ……………………… {since θ/t = ω}

Relation Between Linear Acceleration And Angular Acceleration
Suppose an object rotating about a fixed axis, changes its angular velocity by Δω in Δt. Then the change in tangential velocity, ΔVt, at the end of this interval is
ΔVt = r Δω
Dividing both sides by Δt, we get
ΔVt / Δt = r Δω / Δt
If the time interval is very small i.e., Δt → 0 then

Alternate Method
Linear acceleration of a body is given by
a = (Vr – Vi) / t
But Vr = r ω r and Vi = r ω i
Therefore,
a = (r ω r – r ω i) / t
=> a = r (ωr- ωi) / t
a = r α ……………………………… {since (ωr = ωi) / t = ω}

Time Period
When an object is rotating in a circular path, the time taken by it to complete one revolution or cycle is called its time period, (T).
We know that
ω = Δθ / Δt OR Δt = Δθ / ω
For one complete rotation
Δθ = 2 π
Δt = T
Therefore,
T = 2 π / ω
If ω = 2πf …………………… {since f = frequency of revolution}
Therefore,
T = 2π / 2πf
=> T = 1 / f

Tangential Velocity
When a body is moving along a circle or circular path, the velocity of the body along the tangent of the circle is called its tangential velocity.
Vt = r ω
Tangential velocity is not same for every point on the circular path.

Centripetal Acceleration
A body moving along a circular path changes its direction at every instant. Due to this change, the velocity of the body ‘V’ is changing at every instant. Thus body has an acceleration which is called its centripetal acceleration. It is denoted by a(c) or a1 and always directed towards the centre of the circle. The magnitude of the centripetal acceleration a(c) is given as follows
a(c) = V2 / r, ……………………… r = radius of the circular path

Prove That a(c) = V2 / r

Proof
Consider a body moving along a circular path of radius of r with a constant speed V. Suppose the body moves from a point P to a point Q in a small time Δt. Let the velocity of the body at P is V1 and at Q is V2. Let the angular displacement made in this time be ΔO .
Since V1 and V2 are perpendicular to the radial lines at P and Q, therefore, the angle between V1 and V2 is also Δ0, Triangles OPQ and ABC are similar.
Therefore,
|ΔV| / |V1| = Δs / r
Since the body is moving with constant speed
Therefore,
|V1| = |V2| = V
Therefore,
ΔV / V = Vs / r
ΔV = (V / r) Δs
Dividing both sides by Δt
Therefore,
ΔV / Δt = (V/r) (V/r) (Δs / Δt)
taking limit Δt → 0.

Proof That a(c) = 4π2r / T2

Proof
We know that
a(c) = V2 / r
But V = r ω
Therefore,
a(c) = r2 ω2 / r
a(c) = r ω2 …………………. (1)
But ω = Δθ / Δt
For one complete rotation Δθ = 2π, Δt = T (Time Period)
Therefore,
ω = 2π / T
(1) => a(c) = r (2π / T)2
a(c) = 4 π2 r / T2 ……………… Proved

Tangential Acceleration
The acceleration possessed by a body moving along a circular path due to its changing speed during its motion is called tangential acceleration. Its direction is along the tangent of the circular path. It is denoted by a(t). If the speed is uniform (unchanging) the body do not passes tangential acceleration.
Total Or Resultant Acceleration
The resultant of centripetal acceleration a(c) and tangential acceleration a(t) is called total or resultant acceleration denoted by a.

Centripetal Force
If a body is moving along a circular path with a constant speed, a force must be acting upon it. Direction of the force is along the radius towards the centre. This force is called the centripetal force by F(c).
F(c) = m a(c)
F(c) = m v(2) / r ………………… {since a(c) = v2 / r}
F(c) = mr2 ω2 r ………………….. {since v = r ω}
F(c) = mrω2

Princess Flavia

Princess Flavia
Introduction
Princess Flavia is a character from the novel entitled The Prisoner of Zenda, written by Anthony Hope. She is the only female character who is not directly involved in the conspiracies, which pervade the entire atmosphere of the novel. She is the cousin and fiancée of King Rudolf Elphberg and is the immediate inheritor to the throne. She bears a bewitching personality and fascinates the readers by the elegant attitude.

Her appearance can be perceived by Rudolf Rassendyll’s saying:

“A girl pale and lovely, surmounted by a crown of glorious Elphberg hair.”
Beautiful Aspects of her Role
Princess Flavia is a young, captivating and decent lady. She possesses a character full of virtues and commands great respect and admiration among the people of Ruritania. They wish to see her as the future queen of the country. She is a noble and kind-hearted woman.
“Trust men, and they will be true to you; treat them greatly, and they will show themselves great.”
- Ralph Waldo Emerson

Soberness and Intelligence
Princess Flavia is a wise woman. Her wisdom keeps her aware of the evil desires of Black Michael, who is not a good man. She very intelligently keeps herself away from all sorts of intrigues. She is a sensible person who has the courage to face the realities of life.
Her intelligence is enlightened when she said to Rassendyll:

“Do be careful,” she went on, “you don’t – indeed you don’t – keep enough watch on him.”
Romance
Princess Flavia is a lady with elements of love in her heart. These elements increase the fascination and temptation in her character. She sincerely and quite confidently admits her inclination towards Rassendyll, being impressed by his personality. She was bold enough to propose Rassendyll but her sensibility restricted her to perform any action below dignity. She gave heart and soul to Rudolf Rassendyll considering him to be the real king. She never mourns her decision even after coming to know that he is a pretender. She confessed that Rudolf Rassendyll was acceptable to him even if he was a beggar.
“The fate of love is that it always seems too little or too much.”
- Amelia Barr

Devotion
The princess was a sincere and devoted lady, always worried about the security of Rassendyll. She advised him time and again to be cautious of the wicked plans of Duke Michael. When Black Michael was successful in injuring Rassendyll, she at once reached Zenda to look after him. This action reflects her sense of responsibility and devotion towards the man whom she loved from the depths of her heart.
She said to Rassendyll:
“Oh, if you were not the king, then I could show you how I love you.”
Duty and Patriotism
Princess Flavia is a responsible lady. She very loyal to her country and knows the difference between love and duty. She sets an example of the greatest sacrifice by giving up her love at the altar of duty. This aspect of her character shows that she is not the slave of her passions.
Here sense of duty is enlightened when she says to Rassendyll:
“Your ring will always be on my finger, your heart in my heart. But you must go and I must stay.”
The Great Sacrifice
In order to maintain peace in Ruritania and not to disgrace the royal family, Princess Flavia took a sensible and daring step. She sacrificed her love for the sake of her homeland and parted with Rassendyll forever. It was a noble and graceful decision in the interest of Ruritania and the Royal family.
“There is no moral authority like that of sacrifice.”
– Nadine Gordimer
Conclusion
Princess Flavia proves to be not only the leading female character of the novel but also the most lively and integral personality. She holds the attentions of the readers because of her charm, duty and incredible virtues. She respected the wishes of the people and the country and gave up her love for the sake of her country. She is a complete symbol of love, beauty and sacrifice, which makes her an admirable character.

To love one person with a private love is poor and miserable, to love all is glorious.”


..................................

Thursday, 18 September 2014

Gravitation - 1st Year Physics

Gravitation - 1st Year Physics

    Gravitation

    The property of all objects in the universe which carry mass, by virtue of which they attract one another, is called

Gravitation.

    Centripetal Acceleration of the Moon

    Newton, after determining the centripetal acceleration of the moon, formulated the law of universal gravitation.
    Suppose that the moon is orbiting around the earth in a circular orbit.
    If V = velocity of the moon in its orbit,
    Rm = distance between the centres of earth and moon,
    T = time taken by the moon to complete one revolution around the earth.
    For determining the centripetal acceleration of the moon,. Newton applied Huygen’s formula which is
    a(c) = v2 / r
    For moon, am = v2 / Rm ………………… (1)
    But v = s/t = circumference / time period = 2πRm/T
    Therefore,
    v2 = 4π2Rm2 / T2
    Therefore,
    => a(m) = (4π2Rm2/T2) x (1/Rm)
    a(m) = 4π2Rm / T2
    Put Rm = 3.84 x 10(8) m
    T = 2.36 x 10(6) sec
    Therefore,
    a(m) = 2.72 x 10(-3) m/s2

    Comparison Between ‘am’ AND ‘g’
    Newton compared the centripetal acceleration of the moon ‘am’ with the gravitational acceleration ‘g’.
    i.e., am / g = 1 / (60)2 …………….. (1)
    If Re = radius of the earth, he found that
    Re2 / Rm2 – 1 / (60)2 ……………………. (2)
    Comparing (1) and (2),
    am / g = Re2 / Rm2 ………………………………. (3)
    From equation (3), Newton concluded that at any point gravitational acceleration is inversely to the square of the distance

of that point from the centre of the earth. It is true of all bodies in the universe. This conclusion provided the basis for the

Newton’ Law of Universal Gravitation.

    Newton’s Law of Universal Gravitation

    Consider tow bodies A and B having masses mA and mB respectively.


    Let,
    F(AB) = Force on A by B
    F(BA) = Force on B by A
    r(AB) = displacement from A to B
    r(BA) = displacement from B to A
    r(AB) = unit vector in the direction of r(AB).
    r(BA) = unit vector in the direction of r(BA).

    From a(m) / g = Re2 / Rm2, we have
    F(AB) ∞ 1 / r(BA)2 ……………………. (1)
    Also,
    F(AB) ∞ m(A) …………………………. (2)
    F(BA) ∞ m(B)
    According to the Newton’s third law of motion
    F(AB) = F(BA) ……………….. (for magnitudes)
    Therefore,
    F(AB) ∞ m(B) ………………………….. (3)
    Combining (1), (2) and (3), we get
    F(AB) ∞ m(A)m(B) / r(BA)2
    F(AB) = G m(A)m(B) / r(BA)2 ……………………… (G = 6.67 x 10(-11) N – m2 / kg2)

    Vector Form
    F(AB) = – (G m(A)m(B) / r(BA)2) r(BA)
    F(BA) = – (G m(B)m(A) / r(AB)22) r(AB)
    Negative sign indicates that gravitational force is attractive.

    Statement of the Law
    “Every body in the universe attracts every other body with a force which is directly proportional to the products of their

masses and inversely proportional to the square of the distance between their centres.”

    Mass and Average Density of Earth

    Let,
    M = Mass of an object placed near the surface of earth
    M(e) = Mass of earth
    R(e) = Radius of earth
    G = Acceleration due to gravity
    According to the Newton’s Law of Universal Gravitation.
    F = G M Me / Re2 ……………………….. (1)
    But the force with which earth attracts a body towards its centre is called weight of that body.


    Therefore,
    F = W = Mg
    (1) => M g = G M Me / Re2
    g = G Me / Re2
    Me = g Re2 / G ……………………………. (2)
    Put
    g = 9.8 m/sec2,
    Re = 6.38 x 10(6) m,
    G = 6.67 x 10(-11) N-m2/kg2, in equation (2)
    (1) => Me = 5.98 x 10(24) kg. ………………. (In S.I system)
    Me = 5.98 x 10(27) gm ……………………………… (In C.G.S system)
    Me = 6.6 x 10(21) tons
    For determining the average density of earth (ρ),
    Let Ve be the volume of the earth.
    We know that
    Density = mass / volume
    Therefore,
    ρ = Me / Ve ……………………… [Ve = volume of earth]
    ρ = Me / (4/3 Π Re3) ………….. [since Ve = 4/3 Π Re3]
    ρ = 3 Me / 4 Π Re3
    Put,
    Me = 5.98 x 10(24) kg
    & Re = 6.38 x 10(6) m
    Therefore,
    ρ = 5.52 x 10(3) kg / m3

    Mass of Sun

    Let earth is orbiting round the sun in a circular orbit with velocity V.
    Me = Mass of earth
    Ms = Mass of the sun
    R = Distance between the centres of the sun and the earth
    T = Period of revolution of earth around sun
    G = Gravitational constant
    According to the Law of Universal Gravitation
    F = G Ms Me / R2 ……………………………… (1)
    This force ‘F’ provides the earth the necessary centripetal force
    F = Me V2 / R …………………………………….. (2)
    (1) & (2) => Me V2 / R = G Ms Me / R2
    => Ms = V2 R / G …………………………………. (3)
    V = s / Π = 2Π R / T
    => V2 = 4Π2 R2 / T2
    Therefore,
    (3) => Ms = (4Π R2 / T2) x (R / G)
    Ms = 4Π2 R3 / GT2 …………………………………. (4)
    Substituting the value of
    R = 1.49 x 10(11),
    G = 6.67 x 10(-11) N-m2 / kg2,
    T = 365.3 x 24 x 60 x 60 seconds, in equation (4)
    We get
    Ms = 1.99 x 10(30) kg

    Variation of ‘g’ with Altitude
    Suppose earth is perfectly spherical in shape with uniform density ρ. We know that at the surface of earth
    g = G Me / Re2
    where
    G = Gravitational constant
    Me = Mass of earth
    Re = Radius of earth
    At a height ‘h’ above the surface of earth, gravitational acceleration is
    g = G Me / (Re + h)2
    Dividing (1) by (2)
    g / g = [G Me / Re2] x [(Re + h)2 / G Me)
    g / g = (Re + h)2 / Re2
    g / g = [Re + h) / Re]2
    g / g = [1 + h/Re]2
    g / g = [1 + h/Re]-2
    We expand R.H.S using Binomial Formula,
    (1 + x)n = 1 + nx + n(n-1) x2 / 1.2 + n(n + 1)(n-2)x3 / 1.2.3 + …
    If h / Re < 1, then we can neglect higher powers of h / Re.

    Therefore

    g / g = 1 – 2 h / Re

    g = g (1 – 2h / Re) …………………………… (3)

    Equation (3) gives the value of acceleration due to gravity at a height ‘h’ above the surface of earth.

    From (3), we can conclude that as the value of ‘h’ increases, the value of ‘g’ decreases.

    Variation of ‘g’ with Depth

    Suppose earth is perfectly spherical in shape with uniform density ρ.

    Let

    Re = Radius of earth

    Me = Mass of earth

    d = Depth (between P and Q)

    Me = Mass of earth at a depth ‘d’

    At the surface of earth,

    g = G Me / Re2 ……………………………….. (1)

    At a depth ‘d’, acceleration due to gravity is

    g = G Me / (Re – d)2 ……………………… (2)

    Me = ρ x Ve = ρ x (4/3) π Re3 = 4/3 π Re3 ρ

    Me = ρ x Ve = ρ x (4/3) π (Re – d)3 = 4/3 π (Re – d)3 ρ

    Ve = Volume of earth

    Substitute the value of Me in (1),

    (1) => g = (G / Re2) x (4/3) π Re3 ρ
    g = 4/3 π Re ρ G …………………………… (3)
    Substitute the value of Me in (2)
    g = [G / Re - d)2] x (4/3) π (Re – d)3 ρ
    g = 4/3 π (Re – d) ρ G
    Dividing (4) by (3)
    g / g = [4/3 π (Re - d) ρ G] / [4/3 π Re ρ G]
    g / g = (Re – d) / Re
    g / g = 1 – d/Re
    g / g = g (1 – d / Re) ……………………… (5)
    Equation (5) gives the value of acceleration due to gravity at a depth ‘d’ below the surface of earth
    From (5), we can conclude that as the value of ‘d’ increases, value of ‘g’ decreases.
    At the centre of the earth.
    d = Re => Re / d = 1
    Therefore,
    (5) => g = g (1-1)
    g = 0
    Thus at the centre of the earth, the value of gravitational acceleration is zero.


    Weightlessness in Satellites

    An apparent loss of weight experienced by a body in a spacecraft in orbit is called weightlessness.
    To discuss weightlessness in artificial satellites, let us take the example of an elevator having a block of mass ;m; suspended

by a spring balance attached to the coiling of the elevator. The tension in the thread indicates the weight of the block.
    Consider following cases.

    1. When Elevator is at Rest
    T = m g

    2. When Elevator is Ascending with an Acceleration ‘a’
    In this case
    T > m g
    Therefore, Net force = T – mg
    m a = T – m g
    T = m g + m a
    In this case of the block appears “heavier”.

    3. When Elevator is Descending with an Acceleration ‘a’
    In this case
    m g > T
    Therefore
    Net force = m g – T
    m a = m g – T
    T = m g – m a
    In this case, the body appears lighter

    4. When the Elevator is Falling Freely Under the Action of Gravity
    If the cable supporting the elevator breaks, the elevator will fall down with an acceleration equal to ‘g’
    From (3)
    T = m g – m a
    But a = g
    Therefore
    T = m g – m g
    T = 0
    In this case, spring balance will read zero. This is the state of “weightlessness”.
    In this case gravitation force still acts on the block due to the reason that elevator block, spring balance and string all have

same acceleration when they fall freely, the weight of the block appears zero.

    Artificial Gravity

    In artificial satellites, artificial gravity can be created by spinning the space craft about its own axis.
    Now we calculate frequency of revolution (v) of a space craft of length 2R to produce artificial gravity in it. Its time period

be ‘T’ and velocity is V.

Torque, Angular, Momentum and Equilibrium - 1st Year Physics

 Torque, Angular, Momentum and Equilibrium - 1st Year Physics

    Torque, Angular, Momentum and Equilibrium


    Torque or Moment of Force -

    Definition

    If a body is capable of rotating about an axis, then force applied properly on this body will rotate it about the axis (axis of

rotating). This turning effect of the force about the axis of rotation is called torque.

    Torque is the physical quantity which produces angular acceleration in the body.

    Explanation
    Consider a body which can rotate about O (axis of rotation). A force F acts on point P whose position vector w.r.t O is r.



    F is resolved into F1 and F2. θ is the angle between F and extended line of r.
    The component of F which produces rotation in the body is F1.
    The magnitude of torgue (π) is the product of the magnitudes of r and F1.
    Equation (1) shows that torque is the cross-product of displacement r and force F.
    Torque → positive if directed outward from paper
    Torque → negative if directed inward from paper
    The direction of torque can be found by using Right Hand Rule and is always perpendicular to the plane containing r & F.
    Thus
    Clockwise torque → negative
    Counter-Clockwise torque → positive

    Alternate Definition of Torque
    π = r x F
    |π| = r F sin θ
    |π| = F x r sin θ
    But r sin θ = L (momentum arm) (from figure)
    Therefore,
    |π| = F L
    Magnitude of Torque = Magnitude of force x Moment Arm

    Note
    If line of action of force passes through the axis of rotation then this force cannot produce torque.
    The unit of torque is N.m.

    Couple
    Two forces are said to constitute a couple if they have
    1. Same magnitudes
    2. Opposite directions
    3. Different lines of action
    These forces cannot produces transiatory motion, but produce rotatory motion.

    Moment (Torque) of a Couple
    Consider a couple composed of two forces F and -F acting at points A and B (on a body) respectively, having position

vectors r1 & r2.
    If π1 is the torque due to force F, then
    π1 = r1 x F
    Similarly if π2 is the torque due to force – F, then
    π2 = r2 x (-F)
    The total torque due to the two forces is
    π = π1 + π2
    π = r1 x F + r2 x (-F)
    π = r1 x F – r2 x (-F)
    π = (r1 – r2) x F
    π = r x F
    where r is the displacement vector from B to A.
    The magnitude of torque is
    π = r F sin (180 – θ)
    π = r F sin θ ……………….. {since sin (180 – θ) = sin θ}
    Where θ is the angle between r and -F.
    π = F (r sin θ)
    But r sin θ is the perpendicular distance between the lines of action of forces F and -F is called moment arm of the couple

denoted by d.
    π = Fd
    Thus
    [Mag. of the moment of a couple] = [Mag. of any of the forces forming the couple] x [Moment arm of the couple]
    Moment (torque) of a given couple is independent of the location of origin.

    Centre of Mass

    Definition
    The centre of mass of a body, or a system of particles, is a point on the body that moves in the same way that a single

particle would move under the influence of the same external forces. The whole mass of the body is supposed to be

concentrated at this point.
    Explanation
    During translational motion each point of a body moves in the same manner i.e., different particles of the body do not

change their position w.r.t each other. Each point on the body undergoes the same displacement as any other point as time

goes on. So the motion of one particle represents the motion of the whole body. But in rotating or vibrating bodies different

particles move in different manners except one point called centre of mass. The centre of mass of a body or a system of

particle is a point which represents the movement of the entire system. It moves in the same way that a single particle would

move under the influence of same external forces.

    Centre of Mass and Centre of Gravity
    In a completely uniform gravitational field, the centre of mass and centre of gravity of an extended body coincides. But if

gravitational field is not uniform, these points are different.

    Determination of the Centre of Mass
    Consider a system of particles having masses m1, m2, m3, …………….. mn. Suppose x1, and z1, z2, z3 are their distances on

z-axis, all measured from origin.

    Equilibrium

    A body is said to be in equilibrium if it is
    1. At rest, or
    2. Moving with uniform velocity
    A body in equilibrium possess no acceleration.

    Static Equilibrium
    The equilibrium of bodies at rest is called static equilibrium. For example,
    1. A book lying on a table
    2. A block hung from a string

    Dynamic Equilibrium
    The equilibrium of bodies moving with uniform velocity is called dynamic equilibrium. For example,
    1. The jumping of a paratrooper by a parachute is an example of uniform motion. In this case, weight is balanced by the

reaction of the air on the parachute acts in the vertically upward direction.
    2. The motion of a small steel ball through a viscous liquid. Initially the ball has acceleration but after covering a certain

distance, its velocity becomes uniform because weight of the ball is balanced by upward thrust and viscous force of the liquid.

Therefore, ball is in dynamic equilibrium.

    Angular Momentum

    Definition
    The quantity of rotational motion in a body is called its angular momentum. Thus angular momentum plays same role in

rotational motion as played by linear momentum in translational motion.
    Mathematically, angular momentum is the cross-product of position vector and the linear momentum, both measured in an

inertial frame of reference.
    ρ = r x P

    Explanation
    Consider a mass ‘m’ rotating anti-clockwise in an inertial frame of reference. At any point, let P be the linear momentum

and r be the position vector.
    ρ = r x P
    ρ = r P sinθ ……….. (magnitude)
    ρ = r m V sinθ ………. {since P = m v)
    where,
    V is linear speed
    θ is the angle between r and P
    θ = 90º in circular motion (special case)
    The direction of the angular momentum can be determined by the Righ-Hand Rule.
    Also
    ρ = r m (r ω) sin θ
    ρ = m r2 ω sin θ

    Units of Angular Momentum
    The units of angular momentum in S.I system are kgm2/s or Js.
    1. ρ = r m V sin θ
    = m x kg x m/s
    = kg.m2/s

    2. ρ = r P sin θ
    = m x Ns
    = (Nm) x s
    = J.s

    Dimensions of Angular Momentum
    [ρ] = [r] [P]
    = [r] [m] [V]
    = L . M . L/T
    = L2 M T-1

    Relation Between Torque and Angular Momentum

    OR

    Prove that the rate of change of angular momentum is equal to the external torque acting on the body.

    Proof
    We know that rate of change of linear momentum is equal to the applied force.
    F = dP / dt
    Taking cross product with r on both sides, we get
    R x F = r x dP / dt
    τ = r x dP / dt ……………………….. {since r x P = τ}
    Now, according to the definition of angular momentum
    ρ = r x P
    Taking derivative w.r.t time, we get
    dρ / dt = d / dt (r x P)
    => dρ / dt = r x dP / dt + dr / dt x P
    => dρ / dt = τ + V x P ……………… {since dr / dt = V}
    => dρ / dt = τ + V x mV
    => dρ / dt = τ + m (V x V)
    => dρ / dt = τ + 0 …………….. {since V x V = 0}
    => dρ / dt = τ
    Or, Rate of change of Angular Momentum = External Torque …………….. (Proved)



WORK, POWER & ENERGY - 1st Year Physics

WORK, POWER & ENERGY - 1st Year Physics

    WORK, POWER & ENERGY


    Work

    Work is said to be done when a force causes a displacement to a body on which it acts.
    Work is a scalar quantity. It is the dot product of applied force F and displacement d.



    W = F . d
    W = F d cos θ ………………………… (1)
    Where θ is the angle between F and d.
    Equation (1) can be written as
    W = (F cos θ) d
    i.e., work done is the product of the component of force (F cos θ) in the direction of displacement and the magnitude of

displacement d.
    equation (1) can also be written as
    W = F (d cos θ)
    i.e., work done is the product of magnitude of force F and the component of the displacement (d cos θ) in the direction of

force.

    Unit of Work
    M.K.S system → Joule, BTU, eV
    C.G.S system → Erg
    F.P.S system → Foot Pound
    1 BTU = 1055 joule
    1 eV = 1.60 x 10(-19)

    Important Cases
    Work can be positive or negative depending upon the angle θ between F and d.

    Case I
    When θ = 0º i.e., when F and d have same direction.
    W = F . d
    W = F d cos 0º ………….. {since θ = 0º}
    W = F d …………………….. {since cos 0º = 1}
    Work is positive in this case.

    Case II
    When θ = 180º i.e., when F and d have opposite direction.

    W = F . d
    W = F d cos 180º ………………………. {since θ = 180º}
    W = – F d ………………………………….. {since cos 180º = -1}
    Work is negative in this case

    Case III
    When θ = 90º i.e, when F and d are mutually perpendicular.
    W = F . d
    W = F d cos 90º ………………………. {since θ = 90º}
    W = 0 ……………………………………. {since cos 90º = 0}

    Work Done Against Gravitational Force
    Consider a body of mass ‘m’ placed initially at a height h(i), from the surface of the earth. We displaces it to a height h(f)

from the surface of the earth. Here work is done on the body of mass ‘m’ by displacing it to a height ‘h’ against the

gravitational force.
    W = F . d = F d cos θ
    Here,
    F = W = m g
    d = h(r) – h(i) = h
    θ = 180º
    {since mg and h are in opposite direction}
    Since,
    W = m g h cos 180º
    W = m g h (-1)
    W = – m g h
    Since this work is done against gravitational force, therefore, it is stored in the body as its potential energy (F.E)
    Therefore,
    P . E = m g h

    Power

    Power is defined as the rate of doing work.
    If work ΔW is done in time Δt by a body, then its average power is given by P(av) = ΔW / Δt
    Power of an agency at a certain instant is called instantaneous power.

    Relation Between Power and Velocity
    Suppose a constant force F moves a body through a displacement Δd in time Δt, then
    P = ΔW / Δt
    P = F . Δd / Δt ………………… {since ΔW = F.Δd}
    P = F . Δd / Δt
    P = F . V …………………………… {since Δd / Δt = V}
    Thus power is the dot product of force and velocity.

    Units of Power
    The unit of power in S.I system is watt.
    P = ΔW / Δt = joule / sec = watt
    1 watt is defined as the power of an agency which does work at the rate of 1 joule per second.
    Bigger Units → Mwatt = 10(6) watt
    Gwatt = 10(9) watt
    Kilowatt = 10(3) watt
    In B.E.S system, the unit of power is horse-power (hp).
    1 hp = 550 ft-lb/sec = 746 watt

    Energy

    The ability of a body to perform work is called its energy. The unit of energy in S.I system is joule.

    Kinetic Energy
    The energy possessed by a body by virtue of its motion is called it kinetic energy.
    K.E = 1/2 mv2
    m = mass,
    v = velocity

    Prove K.E = 1/2 mv2

    Proof
    Kinetic energy of a moving body is measured by the amount of work that a moving body can do against an unbalanced force

before coming to rest.
    Consider a body of mas ‘m’ thrown upward in the gravitational field with velocity v. It comes to rest after attaining height

‘h’. We are interested in finding ‘h’.
    Therefore, we use
    2 a S = vf2 – vi2 ………………………. (1)
    Here a = -g
    S = h = ?
    vi = v (magnitude of v)
    vf = 0
    Therefore,
    (1) => 2(-g) = (0)2 – (v)2
    -2 g h = -v2
    2 g h = v2
    h = v2/2g
    Therefore, Work done by the body due to its motion = F . d
    = F d cos θ
    Here
    F = m g
    d = h = v2 / 2g
    θ = 0º
    Therefore, Work done by the body due to its motion = (mg) (v2/2g) cos0º
    = mg x v2 / 2g
    = 1/2 m v2
    And we know that this work done by the body due to its motion.
    Therefore,
    K.E = 1/2 m v2

    Potential Energy
    When a body is moved against a field of force, the energy stored in it is called its potential energy.
    If a body of mass ‘m’ is lifted to a height ‘h’ by applying a force equal to its weight then its potential energy is given by
    P.E = m g h
    Potential energy is possessed by
    1. A spring when it is compressed
    2. A charge when it is moved against electrostatic force.

    Prove P.E = m g h OR Ug = m g h

    Proof
    Consider a ball of mass ‘m’ taken very slowly to the height ‘h’. Therefore, work done by external force is
    Wex = Fex . S = Fex S cos θ ……………………………. (1)
    Since ball is lifted very slowly, therefore, external force in this case must be equal to the weight of the body i.e., mg.
    Therefore,
    Fex = m g
    S = h
    θ = 0º ……………………. {since Fex and h have same direction}
    Therefore,
    (1) => Wex = m g h cos 0º
    Wex = m g h …………………………………………………………. (2)
    Work done by the gravitational force is
    Wg = Fg . S = Fg S cosθ …………………………………………. (3)
    Since,
    Fg = m g
    S = h
    θ = 180º …………………. {since Fg and h have opposite direction}
    Therefore,
    (3) => Wg = m g h cos 180º
    Wg = m g h (-1)
    Wg = – m g h …………………………………………………………. (4)
    Comparing (2) and (4), we get
    Wg = -Wex
    Or
    Wex = – Wg
    The work done on a body by an external force against the gravitational force is stored in it as its gravitational potential

energy (Ug).
    Therefore,
    Ug = Wex
    Ug = – Wg ………………………… {since Wex = -Wg}
    Ug = -(-m g h) ………………… {since Wg = – m g h}
    Ug = m g h ……………………………………….. Proved

    Absolute Potential Energy
    In gravitational field, absolute potential energy of a body at a point is defined as the amount of work done in moving it

from that point to a point where the gravitational field is zero.

    Determination of Absolute Potential Energy
    Consider a body of mass ‘m’ which is lifted from point 1 to point N in the gravitational field. The distance between 1 and N

is so large that the value of g is not constant between the two points. Hence to calculate the work done against the force of

gravity, the simple formula W = F .d cannot be applied.
    Therefore, in order to calculate work done from 1 to N, we divide the entire displacement into a large number of small

displacement intervals of equal length Δr. The interval Δr is taken so small that the value of g remains constant during this

interval.
    Diagram Coming Soon
    Now we calculate the work done in moving the body from point 1 to point 2. For this work the value of constant force F

may be taken as the average of the forces acting at the ends of interval Δr. At point 1 force is F1 and at point 2, force is F2.

    Law of Conservation of Energy

    Statement
    Energy can neither be created nor be destroyed, however, it can be transformed from one form to another.

    Explanation
    According to this law energy may change its form within the system but we cannot get one form of energy without spending

some other form of energy. A loss in one form of energy is accompanied by an increase in other forms of energy. The total

energy remains constant.

    Proof
    For the verification of this law in case of mechanical energy (Kinetic and potential energy). Let us consider a body of mass

‘m’ placed at a point P which is at a height ‘h’ from the surface of the earth. We find total energy at point P, point O and

point Q. Point Q is at a distance of (h-x) from the surface of earth.

Princess Flavia - Character Sketch - 2nd Year English

Princess Flavia - Charater Sketch - 2nd Year English

    Princess Flavia
    Introduction
    Princess Flavia is a character from the novel entitled The Prisoner of Zenda, written by Anthony Hope. She is the only

female character who is not directly involved in the conspiracies, which pervade the entire atmosphere of the novel. She is

the cousin and fiancée of King Rudolf Elphberg and is the immediate inheritor to the throne. She bears a bewitching

personality and fascinates the readers by the elegant attitude.

    Her appearance can be perceived by Rudolf Rassendyll’s saying:

    “A girl pale and lovely, surmounted by a crown of glorious Elphberg hair.”
    Beautiful Aspects of her Role
    Princess Flavia is a young, captivating and decent lady. She possesses a character full of virtues and commands great respect

and admiration among the people of Ruritania. They wish to see her as the future queen of the country. She is a noble and

kind-hearted woman.
    “Trust men, and they will be true to you; treat them greatly, and they will show themselves great.”
    - Ralph Waldo Emerson

    Soberness and Intelligence
    Princess Flavia is a wise woman. Her wisdom keeps her aware of the evil desires of Black Michael, who is not a good man.

She very intelligently keeps herself away from all sorts of intrigues. She is a sensible person who has the courage to face the

realities of life.
    Her intelligence is enlightened when she said to Rassendyll:

    “Do be careful,” she went on, “you don’t – indeed you don’t – keep enough watch on him.”
    Romance
    Princess Flavia is a lady with elements of love in her heart. These elements increase the fascination and temptation in her

character. She sincerely and quite confidently admits her inclination towards Rassendyll, being impressed by his personality.

She was bold enough to propose Rassendyll but her sensibility restricted her to perform any action below dignity. She gave

heart and soul to Rudolf Rassendyll considering him to be the real king. She never mourns her decision even after coming to

know that he is a pretender. She confessed that Rudolf Rassendyll was acceptable to him even if he was a beggar.
    “The fate of love is that it always seems too little or too much.”
    - Amelia Barr

    Devotion
    The princess was a sincere and devoted lady, always worried about the security of Rassendyll. She advised him time and

again to be cautious of the wicked plans of Duke Michael. When Black Michael was successful in injuring Rassendyll, she at once

reached Zenda to look after him. This action reflects her sense of responsibility and devotion towards the man whom she

loved from the depths of her heart.
    She said to Rassendyll:
    “Oh, if you were not the king, then I could show you how I love you.”
    Duty and Patriotism
    Princess Flavia is a responsible lady. She very loyal to her country and knows the difference between love and duty. She

sets an example of the greatest sacrifice by giving up her love at the altar of duty. This aspect of her character shows that she

is not the slave of her passions.
    Here sense of duty is enlightened when she says to Rassendyll:
    “Your ring will always be on my finger, your heart in my heart. But you must go and I must stay.”
    The Great Sacrifice
    In order to maintain peace in Ruritania and not to disgrace the royal family, Princess Flavia took a sensible and daring step.

She sacrificed her love for the sake of her homeland and parted with Rassendyll forever. It was a noble and graceful decision

in the interest of Ruritania and the Royal family.
    “There is no moral authority like that of sacrifice.”
    – Nadine Gordimer
    Conclusion
    Princess Flavia proves to be not only the leading female character of the novel but also the most lively and integral

personality. She holds the attentions of the readers because of her charm, duty and incredible virtues. She respected the

wishes of the people and the country and gave up her love for the sake of her country. She is a complete symbol of love,

beauty and sacrifice, which makes her an admirable character.

    To love one person with a private love is poor and miserable, to love all is glorious.”

Rudolf Rassendyll - Character Sketch - 2nd Year English

Rudolf Rassendyll - Character Sketch - 2nd Year English

    Rudolf Rassendyll


    Introduction
    Rudolf Rassendyll is the hero and central character of the novel entitled The Prisoner of Zenda, written by Anthony Hope.

The integral character of Rassendyll holds the attention of the readers throughout the exciting events of the novel. Rassendyll

possesses a prime personality and is linked with the main incidents of the novel in one way or the other.


    Various Aspects of His Role
    Rudolf Rassendyll is a tall, young and handsome man, who belongs to a noble family in England. He is an educated man of

twenty-nine, who has perfect command over German and French. He is bold, cultural and knows the art of becoming popular.

He has red hair, straight nose, blue eyes and a beard. His physical appearance bears striking resemblance to that of the real

king, though there were some points of differences. Rassendyll himself pointed out:
    “The king’s face was slightly more fleshy than mine, the oval of its contour the least trifle more pronounced and his mouth

lacking something of the firmness which was to be gathered from my close-shutting lips.”

    However, in spite of these differences, Colonel Sapt could not help mentioning to Rassendyll:
    “You’re an Elphberg, every inch of you.”


    Adventure
    Rudolf Rassendyll is very fond of adventures and loves to roam about instead of sticking to a job. He is also a good

mastermind who handles difficult situations seeming effortless. The desire to participate in sensational events is always there

in his heart. This desire was fulfilled by his play-acting of King Rudolf Elphberg, who was very identical to him. His likeness

with the king of Ruritania helped him to make his mission a success. He pledges in strong and unequivocal terms:
    “I have been an imposter for the profit of another, but I will not be one for my own; and if the king is not alive and on his

throne before the day of betrothal comes I will tell the truth, come what may.”


    Wisdom and Prudence
    Rudolf Rassendyll proves himself to be a man of outstanding attributes and full of wisdom. He plays the role of the king very

intelligently. Once he gets entangled in Ruritanian politics, he becomes conscious not only of the significance of his royal

position but also of the responsibility, which lies on his shoulders. He is a wise, cool minded and responsible man.


    Faithfulness and Sincerity
    Rudolf Rassendyll is a sincere man. He does not want to keep the throne to himself. He carries out all his responsibilities

with firmness and confidence. He realizes that it is his duty to restore the real king to the throne and he never tries to take

undue advantage as a pretender. His veracity and sincerity is outstanding as he declares:
    “If I’m found out, I’ ll make a clean breast of it, and fight it out with the Duke.”


    Boldness and Courage
    Rudolf Rassendyll is supposed to be gifted with extraordinary courage and chivalry, and does not fall short of our

expectations in this matter. He is an expert rider and an excellent sword man. When time and fate offered Rassendyll a

challenge, he accepted him as a brave man. His stay in Ruritania unfolds his marvelous sense of responsibility, boldness and

wisdom. The role played by him in Ruritania to save the throne from Black Michael was really an act of gallantry and wisdom.


    Romance
    The romantic aspect of Rassendyll’s personality shows that his heart throbs for Princess Flavia but the sense of duty and

devotion to the throne is far stronger in him. The circumstances urge him to express love to Princess Flavia but bot to feel it.

Being deeply conscious of his responsibility and dedication, he declares:
    “I had to keep the princess devoted to me and yet indifferent to me; I had to show affection for her and not feel it.”


    The Great Sacrifice
    In order to maintain peace in Ruritania and not to disgrace the royal family, Rudolf Rassendyll took a sensible and daring

step. He sacrificed his love at the altar of duty and left Ruritania with tears of regret in the eyes of Princess Flavia, words of

gratitude on the lips of king, applause and appreciation from all the countrymen and feeling of satisfaction on his own part.
    “There is no moral authority like that of sacrifice.”
    – Nadine Gordimer

Wednesday, 17 September 2014

Black Michael - Charater Sketch - 2nd Year English

Black Michael - Charater Sketch - 2nd Year English

    Black Michael



    Introduction
    Black Michael is the villain of the novel entitled The Prisoner of Zenda created by Anthony Hope. He is stepbrother of King Elphberg. He is not the legal heir to the throne because he

is the son of the king’s second and morganatic marriage.
    Black Michael is the owner of castle of Zenda and the surrounding estate. Being the favourite of the late king of Ruritania, he was appointed as the Duke of Strelsau. He is schemer and

evil by nature.


    Selfish and Hypocrite
    Black Michael is a selfish man. He loves Princess Flavia just to get the throne. He is a hypocrite and makes a false show of love towards Madam Mauban. He has become popular among

a small number of people of the country by his hypocrisy. He is over ambitious and greedy.


    A Wicked Person
    Black Michael is a sinful man. He makes plot to get the throne with the help of his companions, but always tries to delude them. That is why his followers betray him, when he is

expecting complete victory. He invites Rassendyll to the Summer House through a conspiracy, but fortunately Rassendyll survives. This sharp and evil act shows his wickedness.


    A Cruel Man
    Black Michael is indeed a cruel person. When the king has been in his noose, he treats him in a very harsh and inhuman manner. He does not feel pity for his brother even. Black

Michael is a coward man. He wants to save his life at any cost. He does not come out to handle the situation at any time.


    A Cool-Minded Criminal
    Black Michael is a wicked but a cool minded and genius criminal. When he sees that Rassendyll has impersonated the king of Ruritania he does not make it known to the people to keep

his villainy secret. We see that even Rupert’s interest and love for Mauban do not irritate him. It shows that he is a controlled emotion criminal.


    A Slave of Lust for Power
    Black Michael becomes utterly blind for power. At any rate he wants to usurp the sovereignty form his brother. His lust for power corrupts him and brings his decline.


    The Tragic End
    Black Michael always deceives his close companions. That is why he is killed by one of his own followers. Thus, the villain of the novel receives a tragic end.


Tuesday, 16 September 2014

Character Sketch - The Count of Monte Cristo - 1st Year English

Character Sketch - The Count of Monte Cristo - 1st Year English
Introduction

The Count of Monte Cristo is the hero of the play, The Count’s Revenge. He is the charming, swashbuckling and ever obliging nobleman, splendidly dressed. The handsome hero, gay, cynical, not very young, with the touch of the devil about him.

As A Young Sailor

As a young man, Monte Cristo was known as Edmond Dantes, a mere sailor of Marseilles, a port in South of France. He loved a beautiful Catalan girl, Mercedes, to whom he was engaged. He was to marry her, on his return from a voyage, which he was to undertake in due course of time.

A Victim Of Conspiracy

But the marriage never took place, as a young fisherman, Fernand Mondego, a friend of Edmond and a snake under grass has other plans. Fernand Mondego secretely loved Mercedes and wished to marry her. So the crafty Fernand, hatched the most devilish of plots against his own friend (Edmond) whereby he got him condemned as a spy of exiled Buonopart, by giving false evidence in the court.

Convicted As A Spy

Poor Edmond, a victim of hatred and jealousy, is convicted as a spy and condemned to life imprisonment in an underground dungeon. The evil Fernand then, convinced Mercedes, through false news in the press that Edmond Dantes had died in prison. Then he gradually gained her confidence by sympathizing with her. In this way, Fernand succeeded in marrying Mercedes.

Escapes From Prison

The unfortunate Edmond Dantes, remained in Prison for 14 long years. He is an innocent victim of blind justice. Then luck favoured him. Six years before the events of our play, Edmond contrived to escape from prison. After escaping from prison, he re-establishes himself in life with wonderful speed and success. In six years, he acquires wealth, a little and a dazzling place in the French Society and settles down in Paris.

As Count Of Monte Cristo

As Count of Monte Cristo, he is greatly respected and admired. But his main aim in life is to take revenge from Fernand Mondego, his deadly enemy, now living in Paris as the Count of Morcerf. Monte Cristo discovers after searching investigations, that his old enemy the Count of Morcerf committed yet another gross act of villainy during his service in the French Army. That he accepted bribes from the Turks, with whom France was at war and surrendered the Fortress of Yanina to them, in 1823.

Count’s Revenge

By keeping in the background, Monte Cristo condemns Count of Morcerf as a traitor to his country. He thus succeeds in taking sweet revenge from his archenemy. He first publishes articles in the newspapers and later in the Chamber of Deputies, he backs his charges by giving convincing proofs. It is at this point, in the play, that Morcerf is, at least exposed as the Villain that he is.

Monte Cristo’s Challenge

Albert, the son of the Count of Morcerf is much offended on learning that his own friend is the cause of his family disgrace and disrepute. In a fit of rage, he challenges Monte Cristo to a duel, which was to be fought at Bois-de-Vincennes at 8 a.m.

Duel Averted

Owing to the intervention of the Countess, his beloved of yester-years, Monte Cristo consents to spare her son’s life. Monte Cristo gives his word that Albert would come to no harm and that he would die, in his place. However, it is the villain who dies and Monte Cristo is thus avenged.

Conclusion

There is no denying that Monte Cristo is the pivot around whom the whole play revolves. He is indeed a man of integrity and honour. He has a charming personality. He is kind and noble who is rewarded in the end for his virtuosity.

Character Sketch - The Count of Morcerf - 1st Year English


Character Sketch - The Count of Morcerf - 1st Year English
Introduction

The Count of Morcerf is presented as the villain of the play, The Count’s Revenge. Prior to becoming a Count, he was a fisherman. He was then known as Fernand Mondego. At that point of time, he lived in Marseilles. He had a friend, Edmond Dantes, who was a sailor. Fernand was quite friendly with him. Edmond was engaged to a beautiful Catalan girl, Mercedes. This fact was known to Fernand. But being an evil natured man, he secretly yearned to marry Mercedes. Therefore, to make his dream come true, he hatched a plot – the most diabolic, which any man could have hatched, against any man.

A Rogue And A Rascal

He is out and out a rogue and a rascal. In order to win the hand of Mercedes, he framed a false charge against his friend, Edmond in the court. He proved that Edmond was the spy of the exiled Napoleon Bonapart. He provided false evidences against Edmond and thus got him imprisoned for 20 years. In this way, he very cleverly removed the innocent Edmond, out of the way.

A Mean And Degraded Man

Once Edmond Dantes had been taken care of Fernand had little difficulty in trapping Mercedes into his trap. He first convinced Mercedes, of the death of Edmond by publishing the false news of his death in the newspapers. Then appearing as a friend and a sympathizer her first consoled her. And after wining her confidence, he then proposed to marry her. Being heart-broke and lonely, she accepted his offer. Thus, the evil monster, succeeded in his devilish plan.

A Traitor To His Country

Having accomplished all his plans successfully, he decided to settle down in Paris. So, he said good bye to Marseilles. While in Paris, he joined the Army, and after sometime, became a captain in 1822. The French were at war against the Turks. Fernand as Captain was defending the Fortress of Yanina. Being a coward and a mean person, he surrendered the fortress to the Turks on receiving a huge bribe. He however made it appear as though he got defeated. Having acquired tons of wealth, Fernand took his discharge from the Army. He then took the title of the Count and settled in Paris.

As A Liar And A Wicked Person

Having amassed a huge fortune, the count started living like a lord when he is proved as a traitor in the chamber of Deputies, he still kept denying his charges. Even in the face of sound evidence, he kept denying his guilt. He is a liar and a rogue.

A Violent Death

After he is proved a traitor, he is still not remorseful. When he is face to face with Edmond, he pulls out his pistol to shoot him. But Albert, Beauchamp pounce on him, to snatch the pistol from him. In the struggle the pistol goes off and the Count of Morcerf, shoots himself. Thus Monte Cristo is avenged.





Abou Ben Adhem - 1st Year English

Abou Ben Adhem - 1st Year English

Introduction of the Poet

James Henry Leigh Hunt was born in 1784. He was a religious man educated at Christ Hospital. He then became the editor and writer of a newspaper called The Examiner. His early poems are The Story of Remini and Endymion. The earliest poems he wrote were published when he was in school. In English Literature, Leigh Hunt is known for his achievements as an editor, a critic and an essayist and not so much as a poet.

Introduction of the Poem

Abou Ben Adhem is a poem with a religious concept. The poet has conveyed the ideas of happiness, peace and love through easy and flowing rhymed couplets.
“Love is in your heart which is given by God, so give it to others.”
___________________ John Keats

The poem consists of 2 stanzas, which are composed of 11 lines. It also has some archaic words.

Summary

Abou Ben Adhem was a religious person. One night when he was sleeping peacefully in his room, a sparkling light woke him up.
He found out that this bright light was due to the presence of an angel who was writing something in a golden book. Being a pious man, Abou was not afraid of the Angel and the silence in the room made him more courageous. He asked the angel what he was writing in the book. The reply Abou heard was that he was writing the names of all those people who love God. About asked the angel curiously if his name was in the list. The angel replied was negative. He then politely requested the angel to write his name as those people who love God’s fellow men. The angle wrote and disappeared.
The other night, it came again with a still glistening light and displayed the names of people whom God had blessed. Abou Ben Adhem saw that his name was on the top of the list and it led all the rest.

Moral

This poem conducts the idea that we should love humanity and care for people.

“To get love from God, love the board.”

Lucy Gray - 1st Year English

Lucy Gray - 1st Year English


Introduction of the Poet

William Word Worth was born in 1770 at Cockermouth in Lake District. He was educated at Hawkshed Grammar School and then at St. John’s College, Cambridge. His early poems reflect his love for natural beauty, which he expressed in a unique and artificial style. Some of William’s poems are Lyrical Ballads, Poems in Two Volumes and An Evening Walk. William Words Worth is also known for his achievements as a critic.

Introduction of the Poem

Poem entitled Lucy Gray was written in 1799 and published in the second edition of “Lyrical Ballads.” It tells us the story of a simple tragedy in a cold bleak countryside. The poem has a steady and regular rhythm as a longer lines rhyme together as well as the shorter lines rhyme with each other. The language of the ballad is plain and simple.

Summary

Lucy Gray was a beautiful little girl who lived in a wild moor with her parents. Their house was located in the countryside far away from the cities. Nobody neighbored their house and Lucy lived without having any friends and playmates.
In Western countryside, it is said that if the moon is clearly seen during daylight, a storm appears in that area. One-day Lucy’s mother went town for shopping in the noon. After a while, he father realized that the moon can be seen and predicted a storm in few hours. He quickly told Lucy to take a lantern and go to the town to help her mother. Lucy obeyed her father and was on her way to the city.
Unfortunately, the storm appeared as soon as Lucy left for the town. It started to snow thickly that made it difficult for Lucy to see through. As she was wandering in the snowy atmosphere, she fell in a crevice and died. Her mother somehow returned home at night.
When the little girl did not come back, her parents went out in the snowy mountains shouting for their daughter, but they never found Lucy. On their way home, they found footprints on a wooden bridge in the middle. They concluded that perhaps Lucy Gray fell down and had died.
When we go through the hills, a solitary song is heard in the wind, which echoes in the mountains. Some people think that she died that day while some say she lives as a part of nature.

....................

 
Design by Free WordPress Themes | Bloggerized by Lasantha - Premium Blogger Themes | Hot Sonakshi Sinha, Car Price in India