Writing a class speech for your 5^th or 6^th grader may not be quite as easy as it sounds! You will have to pack in enough information to make it worthwhile, while retaining the flow and wit to make it interesting to a group of youngsters. Daunting-at the least! The good news is that this need not be an uphill task, so long as you keep to the basics. Here are a few pointers that should stand you in good stead when you are writing a speech!

The Basics First- What Kind Of A Speech Are You Writing?

Well, this is the very basic your need to get right. There are a few categories of speeches. Identifying the type you are dealing with will make your job that much easier. So here goes….

• The informative speech-the basic purpose of these speeches is to impart information about the topic. So, you have to gather a lot of details about the topic if you are writing an informative speech. That is of primary importance.

• Persuasive- this is a speech where you aim at convincing a group of people about a certain point. Creative writing for kids isn’t easy when you are dealing with these class speeches. When you are writing a persuasive speech, it always helps if you have the arguments down in the form of points- easier to remember and convince people at the same time.

• Demonstration speeches- these are your typical show and tell kind of stuff.  Writing these speeches is comparatively easy. You just need to ensure that you go with the flow…

Once you’ve decided on the type of speech you are looking at, you are nearly half way through! Now let’s look at a few points that hold true for all speeches, no matter what format you are putting them under!

Writing a Class Speech- Points to Remember

• Keep it short- there is no way you can convince people if you stuff in too many ideas into your speeches. Moreover, you are just going to make it difficult for your kid to remember everything in class! So, keep the ideas down to a maximum of 2 or 3 and you are good to go!

• Keep it easy on the ears- remember, you are not writing an essay-it’s a speech. So, make it as conversational as you possibly can. Here are a  few pointers you might like to try:

#1-Keep the sentences short.

#2-Substitute ’I’m’ for I am etc.

#3-Steer absolutely clear of flowery gibberish that means little to you or any other fifth grader!

#4-Read it aloud before you finalize it. Does it sound ok? If you are too bored to read through to the end, your audience will probably have the same feelings, so start chopping here and there!

• Make It Real

Real facts that appeal to the audience are far more important than a boring repetition of facts! Creative writing for kids should focus on real life experiences and incidents- that is what makes it come alive!

Keep these easy pointers in mind when you are writing the next class speech for your kid- and watch him win all the accolades from a fascinated audience!

Hurrah! we have won the match.

Heigh-ho! this is a very hot day.

Fie, fie! you should not make such mistakes.

Wow! what a nice dress.

Hush! I have missed the train.

Pooh! I am not afraid of snake.

Alas! he is so sick.

Oh! what a pleasant surprise.

Ah! it was really sad.

One Word to Another Word

When a word is joined with another word by a Conjunction; each of the words is generally of the similar parts of speech; such as,

¨      A noun is joined to another noun or pronoun; an adjective to another adjective; a preposition to another preposition; a verb to another verb.

Noun to Noun – Cows and donkeys are both very helpful animals.

Noun to Pronoun – Sam and you have to come for lunch today.

Pronoun to Pronoun – I and you are both right.

Adjective to Adjective – I am upset, but hopeful.

Preposition to Preposition – A bird flies in and through the air.

Verb to Verb – She came and talked to me wisely.

Noun to Noun – She is a fool as well as a dishonest.

Noun to Noun – Is this baby a boy or a girl?

¨      There are few Conjunctions that often go in pairs; such as, either – or; neither – nor; but – also; both – and; but – also; not only – but also.

Noun to Noun – She is neither an unfair nor a dishonest.

Noun to Noun – He is both an unfair and a dishonest.

Adjective to Adjective – She is both wise and talented.

Adjective to Adjective – She is not only wise, but also talented.

Verb to Verb – You should either work or leave.

Adverb to Adverb – You behaved neither kindly nor wisely.

One Sentence to Another Sentence

Among the Conjunctions that join one sentence to another sentence the mostly can be noticed from the below-mentioned examples: -

Verb is that Parts of Speech by means of which an individual or a thing can be said to do something or to be or become something; or to suffer something. Verbs basically indicate some type of action. In other words, by mans of a Verb we can say something about an individual or a thing.

The word or the group of words indicating the thing or the individual is the Subject of the Verb.

We can find out the Subject of a Verb by asking, What is the thing or Who is the person that is, or suffers, or does?

1) Whale is a fish that does not lay eggs.
2) Sam saw tigers in the zoo.
3) The garden is dug by a gardener.

In the first sentence, what thing is told to be a fish that does not lay eggs? A whale. Therefore, the noun whale is the Subject of the Verb ‘is’.

In the second sentence, what person is told to have seen tigers in the zoo? The person Sam. Therefore, the noun Sam is the Subject of the Verb ‘saw’.

In the third sentence, what thing is told to be dug by a gardener? The ground. Therefore, the noun ground is the Subject of the Verb ‘is dug’.

Whenever, the Verb is associated with the subject a Sentence or the main part of a Sentence is formed.

Verb and Object

If we say, “A cat sleeps”, the action indicated by the Verb sleeps ends with the cat. However, if we say, “A cat killed the mouse”, the action meant by killed does not end with the cat, but it passes on to the mouse who is killed.

1)      A cat killed the mouse.

In this sentence, mouse is the Object to the Verb killed.

2) A cat sleeps the mouse.

The sentence makes no sense. The Verb sleeps can’t have an Object after it.

Verbs can be divided into three classes:-

• Transitive
• Intransitive
• Auxiliary

Transitive Verb: – In case of a Transitive Verb, the action does not end with the doer; but the action passes from the doer to the Object. In other words, a Verb that requires an object is a Transitive Verb. For example,

1)      Sam wrote a poem.

2)      I don’t know whether you have come.

In the first example, ‘poem’ is the Object to the Verb ‘wrote’.

In the second example, ‘whether you have come’ is the Object to the Verb ‘know’.

Intransitive Verb: – In case of an Intransitive Verb, the action ends with the doer, instead passes to the Object from the doer. For example,

• We sleep for being fit and healthy.

Sleep what? Has no answer; this is completely non-sense. Objects can’t come after Verbs like sleep. Therefore, sleep is an Intransitive Verb.

Auxiliary Verb: – An Auxiliary Verb helps to form a tense or a mood of another verb; like,

• Did you learn?
• I have slept.
• Does he know?
• We shall overcome.
• You will go.

N.B. – The Verb which is helped by an Auxiliary Verb is called a Principal Verb.

There are few Verbs that without any alteration of form, can be Intransitive or Transitive as per the sense; like

There are some Verbs that have one form for the Intransitive Verb and another form for the Transitive Verb.

Verb that can not be used in all tenses or moods is known as Defective Verb.

Temperature: It is the degree of hotness or coldness of a body; the hotter the body, the higher its temperature. Thus it is different from heat; it is only one of its effects.

Units of heat and temperature: In the S. I. system, the unit of heat is the joule. In the C.G>S> system, it is the calorie. One calorie = 4.2 joules. The corresponding units of temperature are the degree Kelvin (k) in the S.I. system and degree Celsius ⁰C (degree centigrade) in the C.G.S. system. However, the values of a degree is the same i.e. 1 ⁰C = 1 K. In the Fahrenheit scale, the unit of temperature is the degree Fahrenheit (⁰F). The relation between ⁰ C, K and ⁰F is given in the next section.

Thermometers: These are instruments for measuring temperature. Two of the common forms used for elementary study are the Celsius and the Fahrenheit thermometers. Both use mercury as the thermometric substance and both work on the principle that mercury expands equally for equal rises of temperature. In the Celsius thermometer, the two fixed points are 0⁰ C and 100 ⁰ C. The space between the two fixed points is divided into 100 equal parts, each part being a degree Celsius. In the Fahrenheit thermometer, the two fixed points are 32 ⁰ F and 212 ⁰ F. The space between is divided into 180 equal parts, each part forming a degree Fahrenheit (⁰ F).

Conversion from one scale to another:
To convert the ⁰C to ⁰F and vice versa, we can use the formula
F = C × 9 / 5 + 32

This is easy to understand for 100 Celsius divisions occupy the whole space that is occupied by 180 Fahrenheit divisions. So 1⁰ C division is equal to 1 × 180 / 100 or 9 / 5 Fahrenheit divisions. Thus, 10 Celsius divisions will be = 10 × 9 / 5 Fahrenheit divisions.

So a reading of 10⁰ C in the Celsius thermometer will be shown as 10 × 9 / 5 + 32 in the Fahrenheit thermometer. Now instead of 10⁰ C in our example, we can generalize the relation and we get the formula

F = C × 9 / 5 +32

To convert the Celsius reading into the Kelvin scale, we add 273. Thus 20⁰ = (20 + 273) K or 293 K. Conversely, 423 K = (423 – 273 ) ⁰ or 150 ⁰ C. Here we subtract 273 from the Kelvin reading. Why we do so will be clear after we learn gas laws.

This is easy to understand for 100 Celsius divisions occupy the whole space that is occupied by 180 Fahrenheit divisions. So 1⁰ C division is equal to 1 × 180 / 100 or 9 / 5 Fahrenheit divisions. Thus, 10 Celsius divisions will be = 10 × 9 / 5 Fahrenheit divisions. So a reading of 10⁰ C in the Celsius thermometer will be shown as 10 × 9 / 5 + 32 in the Fahrenheit thermometer. Now instead of 10⁰ C in our example, we can generalize the relation and we get the formula
F = C × 9 / 5 +32
To convert the Celsius reading into the Kelvin scale, we add 273. Thus 20⁰ = (20 + 273) K or 293 K. Conversely, 423 K = (423 – 273 ) ⁰ or 150 ⁰ C. Here we subtract 273 from the Kelvin reading. Why we do so will be clear after we learn gas laws.

Different types of thermometers: The thermometer used by doctors is called the clinical thermometer. It is graduated in Fahrenheit degrees, the range being only between 95⁰ F and 110 ⁰ F. This limited range is due to the fact that our body temperature cannot be lower than 95 ⁰ or higher than 110 ⁰ F. In fact our normal temperature is 98.4 ⁰ F. To help read the temperature after taking the instrument from the mouth of the patient, a constriction is provided which prevents the mercury level from going down.

We can however bring it down by giving the thermometer a gentle jerk when it will be ready for use with another patient. Another type of thermometer is the maximum and minimum thermometer which can help us to record the maximum and minimum temperature reached during a certain interval of time, say during the day or night. The description and working of this thermometer can be found in any Physics text book.

The above thermometers depend for their working on the expansion and contraction of mercury on heating. The expansion of metals on heating can also be used for the measurement of temperature Gas thermometers also work on similar principle. The increase in resistance of metals on heating can also provide a basis.

Expansion of Solids: (i) While mercury which is a liquid can expand in volume only, solids can expand in length, area and volume. Expansion in length is called linear expansion, area expansion is known as superficial expansion and volume expansion is cubic expansion.

(ii) While the fact of expansion due to heat is important, scientists and engineers are more interested in the quantitative aspect of it, i.e. how much it expands. This leads us to the concept of expansivity or coefficient of expansion.

Coefficient of linear expansion of a solid i.e. the linear expansivity of the solid.
This is the ratio of the increase in length of a rod to it original length per ⁰ C rise of temperature. It is denoted by the letter alpha ( α ).

Thus we have
α = ( l₂ – l₁ ) / l₁ (t₂ – t₁ )………………(1)
Where l₁ is the length at t₁ ⁰ C, l ₂ is the length at t₂ ⁰ C. α is thus a ratio. Its value for copper is 17 × 10^-6 per ⁰ C. Since it is a ratio, the units of length chosen in the (C.G.S. or S.I units) will not alter its value.

By using the formula () 1 above, we can find any unknown quantity if the others are known. However, formula (2) below which can be deduced from (1) may sometimes be found more useful.

α = ( l₂ – l₁ ) / l₁ (t₂ – t₁ )

Cross multiplying
l₂ – l₁ = α l₁ (t₂ – t₁)
Therefore, l₂ = l₁ + α l₁ (t₂ – t₁)
= l₁ [ 1 + α (t₂ - t₁) ]

i.e. l₂ = l₁ [ 1 + α (t₂ - t₁) ]…………………………………(2)

(iv) Similarly, the coefficients of superficial ( area ) expansion (β) and cubical (volume) expansion (γ) can be written as

A ₂ A₁ [ 1 + α (t₂ - t₁) ]…………………………………….(3)
V ₂ V₁ [ 1 + α (t₂ - t₁) ]…………………………………….(4)

It can be shown that β = 2α and γ = 3α
Thus α for copper is 0.000017 per ⁰ C. Its β and γ values are
2 × 0.000017 per ⁰ C and 3 × 0.000017 per ⁰ C.

To prove β = 2α
We take a square sheet of metal of side unit length. Its area = 1 sq. unit. Suppose it is heated by 1 ⁰ C, each side will now expand and become (1 + α) where α is the coefficient of linear expansion of the metal. The new area is (1 + α) ² i.e. 1 + 2α + α². [α being very small can be neglected]. So the new area becomes 1 + 2α.

Therefore, increase in area = 2α.
And this increase being on unit area for 1 ⁰ C rise of temperature, it is β by definition.
Therefore, we have β = 2 α

To prove γ = 3 α
Let us consider a cube of a metal of side 1 unit of length. Its volume = 1 unit of volume. If it is heated through 1 ⁰ C, each side will expand to (1 + α) and so the new volume will be (1 + α)³ = 1 + 3 α + 3 α² + α³ = 1 + 3 α, as 3 α² and α³ being very small can be neglected. So the increase in volume = 3 α. As this increase is on 1 unit of volume for 1 ⁰ C rise of temperature, it is γ. So we have γ = 3 α.

Newton’s Three Laws of Motion

First Law: All bodies continue to be in a state of rest or of uniform motion in a straight line unless compelled by an external force to act otherwise.

Second Law: Rate of change of momentum is proportional to the impressed force and takes place in the direction in which the force acts.

Third Law: For every action, there is an equal and opposite reaction.

The First Law Explained
(i) Motion is caused or stopped by applying an external force. Without this external force, a body at rest or in motion will remain so for ever. It is this force that brings about the change. This concept thus gives us a definition of force. Force is that, which makes a body move or a moving body stop.

Force, thus tells about the nature of the body – its property by which the body tends to retain its status quo and does not like to be disturbed. This property is known as inertia.

(ii) Examples of the 1st Law: When you travel in a motor car and the latter suddenly stops, you are thrown forward. This is because when the car was in motion, you had the same speed as that of the car, but when it stops moving, you still retain your speed as that of the speeding car, and due to inertia, you still retain that speed for some more time even after it stops. So the position is, although the car has stopped, you still tend to move forward.

A person jumping from a running train is thrown forward and gts badly hurt for a similar reason.

The Second Law of Newton Explained
To understand this, we have first to know the meaning of momentum.

(i) Momentum of a moving body is the quantity of motion possessed by it and is equal to its mass multiplied by its velocity. Thus, we have M = mv, where M is the momentum, m its mass and v is velocity. All moving bodies possess momentum, the amount possessed by them being governed by the above equation.

(ii) The velocity of a body moving with acceleration changes with time and therefore its momentum too changes. Thus if m is the mass of body, u and v the initial and final velocities and t is the time, then mv – mu is the change of momentum in t sec and (mv – mu)/t or m(v – u)/t the rate of change of momentum. Now th 2nd law states that this is α F [the impressed force], i.e.,

m(v – u)/t α F

Things Deductible From The Second Law
(a) (v – u)/t = a (acceleration)

(b) So the above relation becomes

ma α F

or F α ma

which becomes F = ma, if the units are properly chosen.

The above law tells us

(i) Force acting on a mass produces acceleration on it.

(ii) The acceleration produced is proportional to the force.

Thus the second law is also referred to as the law of acceleration.

Definition of force and unit of force:
From the relation F = ma, if m = 1, a = 1, then F is also one. So we can define

(i) Force as that which acting on a mass produces acceleration on it in the direction of the force.

(ii) Unit of force is that force which acting on unit mass produces unit acceleration on it in the direction of the force. I S. I. system, unit of force is newton and in C.G>S. system, it is the dyne.
1 newton (N) = 10⁵ dynes

(iii) Newton: Newton (N) is the S.I. unit of force and is that force which acting on a mass of 1 kg produces on it an acceleration of 1 m/s².

(iv) Dyne is the C.G.S. unit of force which acting on a mass of 1 g produces on it an acceleration of 1 cm/s²
Force is a vector quantity

Like velocity and acceleration, force is a vector quantity. Thus a force of 4 N can be represented by a straight line with an arrow.

——————|——————|——————|—————->

The figure shows a force of 4 N in the direction of the arrow shown.

Newton’s Third Law
There are numerous examples to support Newton’s third law of motion. Following are given few examples.

When we sit on a chair, our weight (force) presses on the seat. The seat in turn simultaneously presses on us. Out pressing on the chain is the action here and the pressing of the seat on us is the reaction.

As a rifle is fired, the bullet moves due to the forward force while the rifle recoils due to an equal backward force.

When we kick a ball, the ball moves forward due to the forward force of our foot, while our foot receives a pressure due to backward force from the ball.

An apple falls on the ground due to the gravitational force of the earth. The apple simultaneously attracts the earth with an equal force. However, the earth does not go up. This is because the force between the earth and apple is very small. This force is enough to pull the apple to the earth but is not enough to pull the earth towards the apple.

Conservation of Momentum
When a moving body A collides with another body B, A loses some of its momentum which the other gains. The gain is equal to the loss; so the total momentum remains unchanged. This principle is known as the law of conservation of momentum. It is understood that no external force comes into play.

If a body A having mass m₁ and velocity u₁ collides with another body B of mass m₂ and velocity u₂ and v₁ and v₂ are their velocities after collision, then
Sum of the initial momenta of the two bodies = m₁ u₁ + m₂ u₂
Sum of the final momenta, i.e., after collision = m₁ v₁ + m₂ v₂
It is found that these two values are equal, i.e.
m₁ u₁ + m₂ u₂ = m₁ u₁ + m₂ u₂

Momentum is a vector quantity. It has both magnitude and direction.
Impulse
Impulse is a force applied for a short time and is represented by F × t, where F is the force and t is the time for which it acts.

For example, a blow or kick is an impulse. The effect of the impulse on the body is that the latter gains in momentum equal to it. Thus if m × v is the gain of momentum, then we have

F × t = mv

Impulse is measured in newton-second (N-s) and momentum in kg-m/s.

Mass And Weight
Any mass possesses weight when it is subject to the influence of gravity. This weight is a force and is equal to m × g. i.e. mass multiplied by acceleration. Here, the acceleration is due to gravity. If mass is 5 kg, then at a place where g = 9.8 m / s², its weight will be 5 × 9.8 newton i.e. 49 N. Conversely, if its weight is 19.6 N, its mass is 19.6/9.8 or 2 kg. Thus mass is matter and weight is a force.

Newton’s Law Of Universal Gravitation
It is known that earth attracts an apple on a tree and the apple too attracts the earth. Newton discovered that this mutual attraction applied not only to earth and apple, but to any two bodies including the heavenly bodies. He stated the law relating to this as follows:

The Law of universal gravitation: Everybody attracts every other body with a force which is directly proportional to the product of the masses and inversely proportional to the square of the distance between them, i.e., F α m₁m₂/r² or F = G m₁m₂/r², where G is the constant of proportionality or the gravitational constant.

As the above law is universal, it is also known as the Law of Universal gravitational and the constant G as universal gravitational constant.

When F is in newton, m₁ and m₂ in kilograms and r in meters, G has the value of 6.67 × 10^-11 SI units i.e. 6.67 × 10^-11 N.m² / kg²
It is easy to see that the above value of G is very, very small.

Let two persons are talking to each other across a table, and each has weights of 50 kg and are separated by 1 meter, then the force of attraction between them will be

F = G × (m₁m₂/r²)
= ( 6.67 × 10^-1 × 50 × 50 ) / 1² = 1.67 × 10^-7 N, which will be many times smaller than the force exerted by a small piece of paper on the pan of a balance. But of the two bodies, if one is the earth which has a large mass and other is you standing on the ground then the mutual force of attraction will not be negligible.

To Determine The Mass Of A Body
(a) Using Newton’s 2nd Law
Suppose you want to find the mass m₁ of body A. Take another body B whose mass m₂ is known.

We subject both m₁ and m₂ to the same force F and note the acceleration on each, say a₁ and a₂. Then we have

F = m₁ a₁ = m₂ a₂
Or m₁/ m₂ = a₂/ a₁

Say a₂/ a₂ = 3
Then we have m₁ / m₂ = 3 ; or m₁ = 3 m₂

We already know m₂
Therefore, m₁ is double that value of m₂
So in this method, the ratio of the accelerations helps you to find the unknown mass.

(b) If m₁ and m₂ are the two masses, the forces of attraction by the earth on them are given by

F₁ = G M_e m₁ / r² and

F₂ = G M_e m₂ / r²
where M_e is the mass of earth.

If F₁ = F₂, then we have

G M_e m₁ / r² = M_e m₂ / r²

Or m₁ = m₂

So the problem is to make earth’s attraction on both of them to be the same.
This is secured by a physical balance.

When we secure the balance and the pointer is in the middle of the scale, earth is attracting both the pans and contents equally. In this condition, the body whose mass m₁ is to be found exactly balances the other body whose mass m₂ is already known.

Weight of a body on earth and on the moon compared:
Suppose the mass of the body is m. It will be the same both on earth and on the moon. Its weight on the earth F_e = G × M_e × m/ r_e² by Newton’s universal law of gravitation. F_e is the weight on earth, M_e mass of earth, m mass of body and r_e radius of earth.

Its weight on the moon F_m = G × M_m × m / r_m²
Dividing (2) by (1), we get F_m / F_e = M_m / M_e × r_e² / r_m²

The mass of earth is about 100 times greater than that of the moon and its radius 4 times.

Hence, F_m / F_e = 1/100 ×4²/1 = 1/6 roughly.

Therefore, weight of body on the moon = F_e / 6 i.e. the weight of the body on the moon is only 1/6 of its weight on earth.

Change in weight due to acceleration and deceleration
When we go up in a lift which is accelerating upwards, we feel heavier, i.e. there is an increase in our weight and when the lift is accelerating downwards, we feel lighter. Why?

In an up-going accelerating lift, the man experiences the same acceleration as the lift say ‘a’ and hence a force ma in the direction of motion where m is the mass of the man. This force by Newton’s third law of motion exerts and equal downward force on the floor of the lift.

Then there is also the force mg – the normal weight of the man’s body pressing on the floor of the lift where g is the acceleration due to gravity. Thus the total or resultant force that the man’s body exerts on the floor is ma + mg or m (g + a) which is more than his normal weight mg. So he feels heavier.

When the lift accelerates downward with the same acceleration ‘a’, part of his normal weight mg is utilized in giving him this acceleration and only the balance is left as his resultant weight which will be mg – ma or m (g – a) and this will be zero when g = a as in free fall.

Weightlessness: Weightlessness is the common experience of the astronaut during most of their journey in space. They feels it during orbital motion, during free fall or where their gravitational weight is balanced or neutralized by an opposing force.

In orbital flight, the weight of the astronaut is just sufficient to provide the centripetal force to keep him in orbit leaving no net force to provide his or her weight. So he feels weightless. In free fall, the acceleration of the astronaut and the capsule is the same namely ‘g’ and in this condition his weight will be zero.

To find an expression for acceleration due to gravity (g) at a given place using Newton’s law of universal gravitation

Let us consider a body of mass ‘m’ on earth.

The force of attraction F on it by the earth is given by

F = G × Mm / r ²

M is the mass of earth, m mass of body and r radius of earth. This force acting on the mass will produce an acceleration ‘g’ on the mass by Newton’s 2nd law.

G = F / M = G. (Mm / r²) / m

= G.M / r²

This acceleration is known as acceleration due to gravity and depends on the mass M of the earth, the distance of the body from the center of the earth (if the body is a few meters high above the earth, this distance can be ignored and r can be taken as the radius of the earth).

Note the value of ‘g’ does not depend on the mass of the body; the formula clearly shows that, for it does not contain ‘m’. Galileo proved this fact by his famous experiment from the leaning tower of Pisa.

Velocity Velocity of a moving body is the rate of change of position of the body in a straight line or the rate of displacement in a given direction. Velocity is expressed as meters per second (m/s). It is a vector quantity.

Vectors: Physical quantities that have both magnitude and direction are known as Vectors.

Vectors are represented by a straight line with an arrow. Examples of vectors are Displacement, Velocity, Acceleration and Force.

Vector quantities are represented by an arrow over them.

A ————1————–1————→ B East

The above figure represents a velocity of 3 meters per second. The magnitude is 3 units of length per second in the direction AB, i.e., East.

Scalars: Quantities that have a magnitude but no direction are known as Scalars. Examples of scalars are Speed, Mass, Volume, Density etc. Suppose a person starts from A and moves along a curved path ACB of distance S meters and reaches B in‘t’ seconds, then the average speed of the person is S/t m/s.

However, the displacement is only AB, which is the straight line distance from A to B that has taken place in ‘t’ seconds. Hence, the velocity of the person is only equal to AB/t m/s, that is very much different from the Speed S/t .

Uniform and variable velocity: Velocity of a moving body is said to be uniform if the body moves equal distances in equal interval of time or if velocity is same at all points of the motion.

On the other hand, if the velocity changes with time, then it is variable velocity.

Acceleration Acceleration is defined as the rate of change of velocity, which means how much the velocity changes per second. Acceleration is said to be uniform if the change of velocity is same throughout. If it is not, then acceleration is variable.

Acceleration is measured in meter per second per second (m/s/s) or in a shorter form m/s². If the velocity increases every second, then the acceleration is positive. If it decreases every second, then it is negative acceleration or retardation.

Motion in a straight line is known as Linear Motion

Equation 1: This equation provides the relation between initial velocity, final velocity, the time taken to reach it, and the acceleration.

Let the initial velocity be u, the final velocity v, time taken t, and acceleration ‘a’, then the change of velocity = v – u

The time taken for this change = t

Therefore, the rate of change of velocity, i.e., change of velocity per sec

or acceleration a = (v – u)/t i.e., v = u + at

Note: If there is retardation, we use ‘–a’ in place of ‘a’.

Equation 2: This equation provides the relation between distance travelled, initial velocity, acceleration and time.

Let the initial velocity be u

Let the final velocity be v

Let the time taken be t

And, let the distance travelled be S

Now S = average velocity × time = [(u + v)/2]/t

But v = u + at {from equation 1}

Substituting for v, we get S = [(u + u + at)/2]×t

= ut + at²/2

Hence, S = ut + at²/2

The same formula can be used for retardation also, but we need to put ‘-a’ in place of ‘a’.

Equation 3: This equation provides the relation between initial velocity, final velocity, acceleration and distance. There is no time factor in it.

v = u + at

Squaring, we get v² = (u + at) ²

= u² + 2uat +a² t²

= u² + 2a (ut + a t²/2)

= u² + 2aS

Hence, v² = u² + 2aS In case of retardation, ‘a’ becomes ‘-a’

Note: To find the distance travelled in a given time, we make use the formula

S = ut + at²/2.

If it is required to find the distance travelled in the third second, then using the formula, we find the distance travelled in 3 sec and in 2 sec and then subtract the value of the second from the first.

However, we can find a single formula to find the distance travelled in the‘t’ th second as given below:

To find the distance travelled in the‘t’ th second

We have to first find the distance in t sec and in (t-1) sec, subtract and simplify. We will get the required formula.

S_t = ut + at²/2, where S_t is the distance travelled in t sec.

S_t-1 = u(t-1) + a(t-1)²/2 where S_t-1 is the distance travelled in t-1 sec.

S_t – S_t-1 = ut + at²/2 – u(t-1) – a(t-1)²/2

i.e., S_’t’th= ut –u(t-1) + a[t² - (t-1)²]/2

= u + a(t² – t²+ 2t – 1)/2

= u + a(2t – 1)/2

= u + a(t – 1/2)
By using the above formula, we can calculate the distance traveled in any particular second.

Thus, when u = 2m/s and a = 0.5 m/s², the distance travelled in the 3rd sec is S_3rd = 2 + 0.5 (3 – 1/2) = 3.25 m

All freely falling bodies are subjected to a uniform acceleration. Its values at the equator and the poles are different. Its value is usually taken to be 9.8 m / s² which is denoted by ‘g’. The three equations of linear motion apply to falling bodies as well. To apply, we have to replace ‘g’ for ‘a’.
Thus the three equations of motion in case of falling bodies are

V = u + gt

If a body is projected upwards, we have to use ‘-g’ for ‘g’.

Example: A body starting from rest and executing an accelerated motion covers a distance of 9 cm in 6 seconds. Calculate (a) the acceleration (b) the final velocity.

(a) S = ut + at²/2

Implies, 9 = (0×6) + (a×6²)/2

Therefore, a = 0.5 m/s²

(b) V = u + at = 0 + (0.5×6) = 3 m/s

A bullet is fired vertically with an initial velocity of 29.4 m/s (a) How high will it reach? (b
) What is the time taken to reach that height?

u = 29.4 m/s; v = 0

g = -9.8 m/s²

S = ?

t = ?

(a) v² = u² + 2gS

Implies, 0 = 29.4² + 2×(-9.8)×S

Implies, S = 2×9.8 = (29.4)²

Implies, S = (29.4)²/(2×9.8) = 44.1 m

(b) v = u + gt

0 = 29.4 + (-9.8) t

Therefore, t = 3 sec

i) My hand is on the table.

In the above sentence, if you omit the word on, then the sentence makes no sense. You can place your hand on the table, or under the table, or above the table. Unless you add some Preposition to the sentence, the relation between the table and the hand is not clear.

ii) You are in a good mood today.

In the sentence, the word in is placed before the noun ‘mood’ (or ‘a good mood’) and shows what you have to do with a good mood. Therefore, in is a Preposition.

iii) You arrived here before me.

In this sentence, the word before is placed before the pronoun ‘me’ and it shows what your arrival has to do with ‘me’. It shows you arrived sooner than I did. Therefore, before is a Preposition.

Prepositions are never added to any Part of Speech other than a noun or a pronoun or their equivalent.

Prepositions often have same form as the Adverbs. So, how can you differentiate? Here is a simple rule that can help you out to solve this problem and that is;

Adverbs are never added to a noun or a pronoun.

Following this rule you can tell whether a word is an Adverb or a Preposition. Some examples are given below;

The noun or the pronoun, which is placed after a Preposition, is called an Object.

• Sometimes two Prepositions are used together, but both having the same object; as,

The rat crept in between the cardboards.

The rat appeared from between the cardboards.

The man stood out from among all.

She came from within her room.

• Sometimes, a Preposition takes form of a phrase, instead of a single word. However, a Prepositional Phrase always ends in a Simple Preposition.

In front of; because of; for the sake of; in the event of, with regard to; on behalf of; with reference to; in the place of; with a view to; on account of; by means of; in opposition to;, because of; in lieu of;, instead of.

• Sometimes, the object to the Preposition is an adverb used as a noun and sometimes is a sentence.

Till then; from here; from now; before now etc. (Adverbs)

She told everybody of what she had done. (Sentence)

What’s Speed Reading?

Well, it is a speedy way of reading text and getting the most out of it. More and more researchers are advocating these techniques to get the most out of reading! Wouldn’t you love to spend less time at your homework-but get the most out of it? Well, the only way out is to read right-and here’s how you go about it!

How Should I Read and Get the Best Out Of It in A Short Time?

• Peace and quiet-The most important thing you need to remember about this is that you should find out the best place for it. For instance, look for peace and quiet-that goes without saying! You can NEVER learn anything without this! Relax-I include your favorite music in the ‘peace and quiet’ I’m talking about!

Having said that, I seriously doubt your powers to concentrate when you are listening to reggae or hard rock at the max! I have nothing against it- but are you sure it helps your concentration?

• Relax as you read-like we told you before, your brain feels pressurized when you task it too much.  Don’t concentrate on cramming facts. Your mind will wander and you will remember precious little!

If you are having problems concentrating- you’re just normal. Why not take up a few minutes of meditation every day? You will find it working miracles! Just about 5 minutes in a day is more than enough at the outset. Surely you can afford that time?

• Plan ahead- you need to be clear about your expectations from the text. For instance, if you are writing an essay and are looking for matter, jot down key words and ideas as you read. You will find it easier to assimilate the ideas later! If you are preparing for a test, this will help you cut down the hours you spend at your table.

• Read in groups- if you read through each word in the text, you will waste time and concentrate less. Instead, try and read the words in groups.

For instance, if you read ‘if you want to concentrate more, read slow’, in individual words, you will just waste time. Instead, why not try and read them like this- ‘if you concentrate more, read slow’! Try it out-it’s fun!

Remember, you need not spend hours at your desk- even before that exam! Just read right and you will get away with the least amount of time-and we all know what you can do with that time! But then, my mind is wandering……
Don’t just do it fast….do it right! Read this quick step

http://tutorteddy.com/wordpress/tips-on-reading-tips-on-writing/4-steps-to-reading-right/

Adverbs can be divided in two categories; 1) Simple Adverbs and 2) Interrogative Adverbs.

1) Simple Adverbs: – Adverbs that simply qualify a Verb, an Adjective or other Adverb are called Simple Adverbs.

Simple Adverbs can be differentiated from each other depending on their meaning;

• Adverbs of Manner or State or Quality: – This type of Adverbs shows in what manner a thing is done or in what state a thing exists; such as,

You did it well. You did it thus (in this way), You did it together. You did the work slowly, but wisely. You all did it alike (the same way). You acted nicely.

N.B: – Adverbs belong to this class often formed by adding ‘ly’ to the Adjectives, like slow, slowly; wise, wisely; nice, nicely, soft, softly; happy, happily; etc.

• Adverbs of Quantity: – This type of Adverbs shows to what extent a thing is done; such as,

You are quite brave. I have almost recovered. You are the only person who did the work.

He is very sick. You have talked enough.

This movie is far the best. I am a little annoyed with you.

I am extremely happy. They are entirely satisfied.

• Adverbs of Numbers: – This type of Adverbs shows in what order or how often a thing is done.

I went there thrice. He came to my house once. He eats four times a day.

I go there sometimes. He often came. You came seldom.

I never went to his house. She came no more to my house. You went there again.

The kid brought firstly a pencil, secondly a chalk and thirdly a slate.

• Adverbs of Time: – This type of Adverbs shows for how long or when a thing is done.

You did this before. I did it afterwards.

I have already done this. You did it long ago.

She was sick then, but is much better now.

You came early but went late. At last you came. I went soon.

You came at once. He has came to-day. They went yesterday.

You have to come hourly. I will go tomorrow.

I go to school daily.

Meanwhile my daughter will stay with me.

• Adverbs of Place: – This type of Adverbs shows in what place or where a thing is done.

She is not here, but there. She was nowhere to be found.

You went backwards, but you should go forwards.

I stood before not behind.

Some of them stood near, others beyond and others around.

We will come here, if you will go there.

You stood aside. I will send you away. I looked for him everywhere.

• Affirming or Denying Adverbs: – This type of Adverbs expresses denying or affirming of something; such as,

I shall surely come. She will probably go.

I answered yes. You answered no. Perhaps they will go.

2) Interrogative Adverbs: – Adverbs that are used for asking some questions are called Interrogative Adverbs; like,

¨      State or Manner: – How did you do this?

¨      Number: – How many days in a week?

¨      Quantity: – How far we have to go?

¨      Time: – How long will they stay here? When did they come?

¨      Place: – Where do you stay?

¨      Cause: – Why did you do that?

N.B: – Sometimes Interrogative Adverbs are used in a Relative sense; these are called Relative Adverbs. The antecedent Noun to which they are related may be either expressed or omitted.

• The antecedent expressed  

This is the house where we stay.

Let me tell you the time when I shall go.

• The antecedent omitted.

This is (= the house in which) where we stay.

Let me tell you when (= the time by which) I shall go.

Sometimes ‘the’ is used as a Relative Adverb; provided it should be place prior to an adverb or an adjective in Comparison Degree and provided a same combination of ‘the’ with a Comparative to come after it. This ‘the’ is distinct from the Definite Article.

The sooner you come, the better for you.

The more you study, the better result you can expect.

The nearer the bone, the sweeter the meat.

In the above sentences, the first ‘the’ is a Relative Adverb, the second ‘the’ is a Simple Adverb.