Gravitation
GRAVITATION
We have learnt about the motion of objects and force as the cause of motion. We have learnt that a force is needed to change the speed or the direction of motion of an object. We always observe that an object dropped from a height falls towards the earth. We know that all the planets go around the Sun. The moon goes around the earth. In all these cases, there must be some force acting on the objects, the planets and on the moon. Isaac Newton could grasp that the same force is responsible for all these. This force is called the gravitational force.
In this chapter we shall learn about gravitation and the universal law of gravitation. We shall discuss the motion of objects under the influence of gravitational force on the earth. We shall study how the weight of a body varies from place to place. We shall also discuss the conditions for objects to float in liquids.
9.1 Gravitation
We know that the moon goes around the earth. An object when thrown upwards, reaches a certain height and then falls downwards. It is said that when Newton was sitting under a tree, an apple fell on him. The fall of the apple made Newton start thinking. He thought that: if the earth can attract an apple, can it not attract the moon? Is the force the same in both cases? He conjectured that the same type of force is responsible in both the cases. He argued that at each point of its orbit, the moon falls towards the earth, instead of going off in a straight line. So, it must be attracted by the earth. But we do not really see the moon falling towards the earth.
Let us try to understand the motion of the moon by recalling activity 7.11.
Activity 9.1
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Take a piece of thread.
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Tie a small stone at one end. Hold the other end of the thread and whirl it round, as shown in Fig. 9.1.
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Note the motion of the stone.
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Release the thread.
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Again, note the direction of motion of the stone.
Fig. 9.1: A stone describing a circular path with a velocity of constant magnitude.
Before the thread is released, the stone moves in a circular path with a certain speed and changes direction at every point. The change in direction involves change in velocity or acceleration. The force that causes this acceleration and keeps the body moving along the circular path is acting towards the centre. This force is called the centripetal (meaning ‘centre-seeking’) force.
In the absence of this force, the stone flies off along a straight line. This straight line will be a tangent to the circular path.
A straight line that meets the circle at one and only one point is called a tangent to the circle. Straight line $ABC$ is a tangent to the circle at point B.
The motion of the moon around the earth is due to the centripetal force. The centripetal force is provided by the force of attraction of the earth. If there were no such force, the moon would pursue a uniform straight line motion.
It is seen that a falling apple is attracted towards the earth. Does the apple attract the earth? If so, we do not see the earth moving towards an apple. Why?
According to the third law of motion, the apple does attract the earth. But according to the second law of motion, for a given force, acceleration is inversely proportional to the mass of an object [Eq. (8.4)]. The mass of an apple is negligibly small compared to that of the earth. So, we do not see the earth moving towards the apple. Extend the same argument for why the earth does not move towards the moon.
In our solar system, all the planets go around the Sun. By arguing the same way, we can say that there exists a force between the Sun and the planets. From the above facts Newton concluded that not only does the earth attract an apple and the moon, but all objects in the universe attract each other. This force of attraction between objects is called the gravitational force.
9.1.1 UNIVERSAL LAW OF GRAVITATION
Every object in the universe attracts every other object with a force which is proportional to the product of their masses and inversely proportional to the square of the distance between them. The force is along the line joining the centres of two objects.
Fig. 9.2: The gravitational force between two uniform objects is directed along the line joining their centres.
Let two objects A and B of masses $M$ and $m$ lie at a distance $d$ from each other as shown in Fig. 9.2. Let the force of attraction between two objects be $F$. According to the universal law of gravitation, the force between two objects is directly proportional to the product of their masses. That is,
$$F \propto M \times m \tag{9.1}$$
And the force between two objects is inversely proportional to the square of the distance between them, that is,
$$ F \propto \frac{1}{d^{2}} \tag{9.2} $$
Combining Eqs. (10.1) and (10.2), we get
$$ F \propto \frac{M \times m}{d^{2}} \tag{9.3} $$
or, $$F=G \frac{M \times m}{d^{2}} \tag{9.4}$$
where $G$ is the constant of proportionality and is called the universal gravitation constant. By multiplying crosswise, Eq. (9.4) gives
$ F \times d^{2}=G M \times m $
$ \text{ or } \quad G=\frac{F d^{2}}{M \times m} $
The SI unit of $G$ can be obtained by substituting the units of force, distance and mass in Eq. (9.5) as $N m^{2} kg^{-2}$.
The value of $G$ was found out by Henry Cavendish (1731 - 1810) by using a sensitive balance. The accepted value of $G$ is $6.673 \times 10^{-11} N m^{2} kg^{-2}$.
We know that there exists a force of attraction between any two objects. Compute the value of this force between you and your friend sitting closeby. Conclude how you do not experience this force!
The law is universal in the sense that it is applicable to all bodies, whether the bodies are big or small, whether they are celestial or terrestrial.
Inverse-square
Saying that $F$ is inversely proportional to the square of $d$ means, for example, that if $d$ gets bigger by a factor of $6, F$ becomes
$\frac{1}{36}$ times smaller.
Example 9.1 The mass of the earth is $6 \times 10^{24} kg$ and that of the moon is $7.4 \quad 10^{22} kg$. If the distance between the earth and the moon is $3.8410^{5} km$, calculate the force exerted by the earth on the moon. (Take $G=6.7 \quad 10^{-11} N m^{2} kg^{-2}$ )
Solution:
The mass of the earth, $M=6 \quad 10^{24} kg$ The mass of the moon,
$ m=7.4 \quad 10^{22} kg $
The distance between the earth and the moon,
$$ \begin{aligned} d & =3.84 \quad 10^{5} km \\ & =3.84 \quad 10^{5} \quad 1000 m \\ & =3.84 \quad 10^{8} m \\ G & =6.7 \quad 10^{-11} N m^{2} kg^{-2} \end{aligned} $$
From Eq. (9.4), the force exerted by the earth on the moon is
$F=G \frac{M \times m}{d^{2}}$
$=\frac{6.7 \times 10^{-11} N m^{2} kg^{-2} \times 6 \times 10^{24} kg \times 7.4 \times 10^{22} kg}{(3.84 \times 10^{8} m)^{2}}$
$=2.02 \times 10^{20} N$.
Thus, the force exerted by the earth on the moon is $2.02 \times 10^{20} N$.
Questions
1. State the universal law of gravitation.
Answer
The universal law of gravitation states that every object in the universe attracts every other object with a force called the gravitational force. The force acting between two objects is directly proportional to the product of their masses and inversely proportional to the square of the distance between their centers.
2. Write the formula to find the magnitude of the gravitational force between the earth and an object on the surface of the earth.
Answer
Let F be the force of attraction between earth and an object on its surface. Again assume that $M_e$ be the mass of earth and $m$ be the mass of object on the surface of earth. Formula for the magnitude of the gravitational force between the earth and an object on the surface of the earth is given by using Universal Law of Gravitation. So required formula is
$F = G\frac{Mm}{r^2}$
9.1.2 IMPORTANCE OF THE UNIVERSAL LAW OF GRAVITATION
The universal law of gravitation successfully explained several phenomena which were believed to be unconnected:
(i) the force that binds us to the earth;
(ii) the motion of the moon around the earth;
(iii) the motion of planets around the Sun; and
(iv) the tides due to the moon and the Sun.
9.2 Free Fall
Let us try to understand the meaning of free fall by performing this activity.
Activity 9.2
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Take a stone.
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Throw it upwards.
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It reaches a certain height and then it starts falling down.
We have learnt that the earth attracts objects towards it. This is due to the gravitational force. Whenever objects fall towards the earth under this force alone, we say that the objects are in free fall. Is there any change in the velocity of falling objects? While falling, there is no change in the direction of motion of the objects. But due to the earth’s attraction, there will be a change in the magnitude of the velocity. Any change in velocity involves acceleration. Whenever an object falls towards the earth, an acceleration is involved. This acceleration is due to the earth’s gravitational force. Therefore, this acceleration is called the acceleration due to the gravitational force of the earth (or acceleration due to gravity). It is denoted by $g$. The unit of $g$ is the same as that of acceleration, that is, $m s^{-2}$.
We know from the second law of motion that force is the product of mass and acceleration. Let the mass of the stone in activity 9.2 be $m$. We already know that there is acceleration involved in falling objects due to the gravitational force and is denoted by $g$. Therefore the magnitude of the gravitational force $F$ will be equal to the product of mass and acceleration due to the gravitational force, that is,
$ F=m g $
From Eqs. (9.4) and (9.6) we have
$$ \begin{aligned} & m g=G \frac{M \times m}{d^{2}} \\ & \text{ or } g=G \frac{M}{d^{2}} \end{aligned} $$
where $M$ is the mass of the earth, and $d$ is the distance between the object and the earth.
Let an object be on or near the surface of the earth. The distance $d$ in Eq. (9.7) will be equal to $R$, the radius of the earth. Thus, for objects on or near the surface of the earth,
$$ \begin{aligned} m g & =G \frac{M \times m}{R^{2}} \\ g & =G \frac{M}{R^{2}} \end{aligned} $$
The earth is not a perfect sphere. As the radius of the earth increases from the poles to the equator, the value of $g$ becomes greater at the poles than at the equator. For most calculations, we can take $g$ to be more or less constant on or near the earth. But for objects far from the earth, the acceleration due to gravitational force of earth is given by Eq. (9.7).
9.2.1 TO CALCULATE THE VALUE OF $g$
To calculate the value of $g$, we should put the values of G, $M$ and $R$ in Eq. (9.9), namely, universal gravitational constant, $G=6.7 \times 10^{-}$ ${ }^{11} N m^{2} kg^{-2}$, mass of the earth, $M=6 \times 10^{24} kg$, and radius of the earth, $R=6.4 \times 10^{6} m$.
$$ \begin{aligned} g & =G \frac{M}{R^{2}} \\ & =\frac{6.7 \times 10^{-11} N m^{2} kg^{-2} \times 6 \times 10^{24} kg}{(6.4 \times 10^{6} m)^{2}} \\ & =9.8 m s^{-2} . \end{aligned} $$
Thus, the value of acceleration due to gravity of the earth, $g=9.8 m s^{-2}$.
9.2.2 MOTION OF OBJECTS UNDER THE INFLUENCE OF GRAVITATIONAL FORCE OF THE EARTH
Let us do an activity to understand whether all objects hollow or solid, big or small, will fall from a height at the same rate.
Activity 9.3
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ake a sheet of paper and a stone. Drop them simultaneously from the first floor of a building. Observe whether both of them reach the ground simultaneously.
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We see that paper reaches the ground little later than the stone. This happens because of air resistance. The air offers resistance due to friction to the motion of the falling objects. The resistance offered by air to the paper is more than the resistance offered to the stone. If we do the experiment in a glass jar from which air has been sucked out, the paper and the stone would fall at the same rate.
We know that an object experiences acceleration during free fall. From Eq. (9.9), this acceleration experienced by an object is independent of its mass. This means that all objects hollow or solid, big or small, should fall at the same rate. According to a story, Galileo dropped different objects from the top of the Leaning Tower of Pisa in Italy to prove the same.
As $g$ is constant near the earth, all the equations for the uniformly accelerated motion of objects become valid with acceleration a replaced by $g$. The equations are:
$$ \begin{aligned} & v=u+a t \\ & s=u t+\frac{1}{2} a t^{2} \\ & v^{2}=u^{2}+2 a s \end{aligned} $$
where $u$ and $v$ are the initial and final velocities and $s$ is the distance covered in time, $t$.
In applying these equations, we will take acceleration, a to be positive when it is in the direction of the velocity, that is, in the direction of motion. The acceleration, a will be taken as negative when it opposes the motion.
Example 9.2 A car falls off a ledge and drops to the ground in $0.5 s$. Let $g=10 m s^{-2}$ (for simplifying the calculations).
(i) What is its speed on striking the ground?
(ii) What is its average speed during the $0.5 s$ ?
(iii) How high is the ledge from the ground?
Solution:
Time, $t=1 / 2$ second
Initial velocity, $u=0 m s^{-1}$
Acceleration due to gravity, $g=10 m s^{-2}$
Acceleration of the car, $a=+10 m s^{-2}$
(downward)
(i) speed
$$ \begin{aligned} V & =a t \\ V & =10 m s^{-2} \times 0.5 s \\ & =5 m s^{-1} \end{aligned} $$
(ii) average speed $=\frac{u+v}{2}$
$$ \begin{aligned} & =(0 m s^{-1}+5 m s^{-1}) / 2 \\ & =2.5 m s^{-1} \end{aligned} $$
(iii) distance travelled, $s=1 / 2 a t^{2}$
$$ \begin{aligned} & =1 / 2 \times 10 m s^{-2} \times(0.5 s)^{2} \\ & =1 / 2 \times 10 m s^{-2} \times 0.25 s^{2} \\ & =1.25 m \end{aligned} $$
Thus,
(i) its speed on striking the ground
$ =5 m s^{-1} $
(ii) its average speed during the $0.5 s$
$ =2.5 m s^{-1} $
(iii) height of the ledge from the ground $=1.25 m$.
Example 9.3 An object is thrown vertically upwards and rises to a height of $10 m$. Calculate (i) the velocity with which the object was thrown upwards and (ii) the time taken by the object to reach the highest point.
Solution:
Distance travelled, $s=10 m$
Final velocity, $v=0 m s^{-1}$
Acceleration due to gravity, $g=9.8 m s^{-2}$
Acceleration of the object, $a=-9.8 m s^{-2}$
(upward motion)
(i) $v^{2}=u^{2}+2 a s$
$$ \begin{aligned} & 0=u^{2}+2 \times(-9.8 m s^{-2}) \times 10 m \\ & -u^{2}=-2 \times 9.8 \times 10 m^{2} s^{-2} \\ & u=\sqrt{196} m s^{-1} \\ & u=14 m s^{-1} \\ & v=u+a t \\ & 0=14 m s^{-1}-9.8 m s^{-2} \times t \\ & t=1.43 s \end{aligned} $$
(ii) $\quad v=u+a t$
Thus,
(i) Initial velocity, $u=14 m s^{-1}$, and
(ii) Time taken, $t=1.43 s$.
Questions
1. What do you mean by free fall?
Answer
Gravity of earth attracts every object towards its center. When an object is dropped from a certain height, it begins to fall towards Earth’s surface under the influence of gravitational force. Such a motion of object is called free fall.
2. What do you mean by acceleration due to gravity?
Answer
When an object falls freely towards the surface of earth from a certain height, then its velocity changes. This change in velocity produces acceleration in the object which is known as acceleration due to gravity denoted by letter $g$. The value of acceleration due to gravity is $g=9.8 m / s^{2}$.
9.3 Mass
We have learnt in the previous chapter that the mass of an object is the measure of its inertia . We have also learnt that greater the mass, the greater is the inertia. It remains the same whether the object is on the earth, the moon or even in outer space. Thus, the mass of an object is constant and does not change from place to place.
9.4 Weight
We know that the earth attracts every object with a certain force and this force depends on the mass $(m)$ of the object and the acceleration due to the gravity $(g)$. The weight of an object is the force with which it is attracted towards the earth.
We know that
$ F=m \times a, $
that is
$ F=m \times g . $
The force of attraction of the earth on an object is known as the weight of the object. It is denoted by $W$. Substituting the same in Eq. (9.14), we have
$ W=m \times g $
As the weight of an object is the force with which it is attracted towards the earth, the SI unit of weight is the same as that of force, that is, newton (N). The weight is a force acting vertically downwards; it has both magnitude and direction.
We have learnt that the value of $g$ is constant at a given place. Therefore at a given place, the weight of an object is directly proportional to the mass, say $m$, of the object, that is, $W \propto m$. It is due to this reason that at a given place, we can use the weight of an object as a measure of its mass. The mass of an object remains the same everywhere, that is, on the earth and on any planet whereas its weight depends on its location because $g$ depends on location.
9.4.1 WEIGHT OF AN OBJECT ON THE MOON
We have learnt that the weight of an object on the earth is the force with which the earth attracts the object. In the same way, the weight of an object on the moon is the force with which the moon attracts that object. The mass of the moon is less than that of the earth. Due to this the moon exerts lesser force of attraction on objects.
Let the mass of an object be $m$. Let its weight on the moon be $W_m$. Let the mass of the moon be $M_m$ and its radius be $R_m$.
By applying the universal law of gravitation, the weight of the object on the moon will be
$ W_m=G \frac{M_m \times m}{R_m^{2}} $
Let the weight of the same object on the earth be $W_e$. The mass of the earth is $M$ and its radius is $R$.
Table 9.1
Celestial | Mass(kg) | Radius(m) |
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Earth | $ 5.98 \times 10^{24}$ | $6.37 \times 10^6$ |
Moon | $7.36 \times 10^{22}$ | $1.74 \times 10^6$ |
From Eqs. (9.9) and (9.15) we have,
$ W_e=G \frac{M \times m}{R^{2}} $
Substituting the values from Table 10.1 in Eqs. (9.16) and (9.17), we get
$$ \begin{gathered} W_m=G \frac{7.36 \times 10^{22} kg \times m}{(1.74 \times 10^{6} m)^{2}} \\ W_m=2.431 \times 10^{10} G \times m \end{gathered} $$
and $W_e=1.474 \times 10^{11} G \times m$
Dividing Eq. (9.18a) by Eq. (9.18b), we get
$$ \begin{aligned} \frac{W_m}{W_e} & =\frac{2.431 \times 10^{10}}{1.474 \times 10^{11}} \\ \text{ or } \frac{W_m}{W_e} & =0.165 \approx \frac{1}{6} \end{aligned} $$
$$ \frac{\text{ Weight of the object on the moon }}{\text{ Weight of the object on the earth }}=\frac{1}{6} $$
Weight of the object on the moon
$$ =(1 / 6) \times \text{ its weight on the earth. } $$
Example 9.4 Mass of an object is $10 kg$. What is its weight on the earth?
Solution:
Mass, $m=10 kg$
Acceleration due to gravity, $g=9.8 m s^{-2}$
$$ \begin{aligned} & W=m \times g \\ & W=10 kg \times 9.8 m s^{-2}=98 N \end{aligned} $$
Thus, the weight of the object is $98 N$.
Example 9.5 An object weighs $10 N$ when measured on the surface of the earth. What would be its weight when measured on the surface of the moon?
Solution:
We know,
Weight of object on the moon
$ =(1 / 6) \times \text{ its weight on the earth. } $
That is,
$$ \begin{aligned} W_m & =\frac{W_e}{6}=\frac{10}{6} N . \\ & =1.67 N . \end{aligned} $$
Thus, the weight of object on the surface of the moon would be $1.67 N$.
Questions
1. What are the differences between the mass of an object and its weight?
Answer
Mass | Weight |
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Mass is the quantity of matter contained in the body | Weigh is the gravitational force acting on the body |
It is the measure of inertia of the body | It is the measure of gravity |
It is a constant quantity for any object. | Weight of an object is not a constant quantity it is different at different laces. |
It is a scalar quantity and only only has magnitude | It is a vector quantity as it has both magnitude and direction. |
SI unit of mass is $Kg$ | Its SI unit is N (newton) same as the SI unit of force. |
2. Why is the weight of an object on the moon $\frac{1}{6}$ th its weight on the earth?
Answer
Gravity is directly related to mass. The more mass an object has, the more gravitational pull it has.
Now, the moon is significantly smaller than the earth (in fact, it is about the size of the earth’s core). Gravity is dependent on the size of the object. Your weight on the moon is $1 / 6$ of that on earth because the moon has $1 / 6$ the mass of the earth.
9.5 Thrust and Pressure
Have you ever wondered why a camel can run in a desert easily? Why an army tank weighing more than a thousand tonne rests upon a continuous chain? Why a truck or a motorbus has much wider tyres? Why cutting tools have sharp edges? In order to address these questions and understand the phenomena involved, it helps to introduce the concepts of the net force in a particular direction (thrust) and the force per unit area (pressure) acting on the object concerned.
Let us try to understand the meanings of thrust and pressure by considering the following situations:
Situation 1: You wish to fix a poster on a bulletin board, as shown in Fig 9.3. To do this task you will have to press drawing pins with your thumb. You apply a force on the surface area of the head of the pin. This force is directed perpendicular to the surface area of the board. This force acts on a smaller area at the tip of the pin.
Fig. 9.3: To fix a poster, drawing pins are pressed with the thumb perpendicular to the board.
Situation 2: You stand on loose sand. Your feet go deep into the sand. Now, lie down on the sand. You will find that your body will not go that deep in the sand. In both cases the force exerted on the sand is the weight of your body.
You have learnt that weight is the force acting vertically downwards. Here the force is acting perpendicular to the surface of the sand. The force acting on an object perpendicular to the surface is called thrust.
When you stand on loose sand, the force, that is, the weight of your body is acting on an area equal to area of your feet. When you lie down, the same force acts on an area equal to the contact area of your whole body, which is larger than the area of your feet. Thus, the effects of forces of the same magnitude on different areas are different. In the above cases, thrust is the same. But effects are different. Therefore the effect of thrust depends on the area on which it acts.
The effect of thrust on sand is larger while standing than while lying. The thrust on unit area is called pressure. Thus,
$ \text{ Pressure }=\frac{\text{ thrust }}{\text{ area }} $
Substituting the SI unit of thrust and area in Eq. (9.20), we get the SI unit of pressure as N/ $m^{2}$ or $N m^{-2}$.
In honour of scientist Blaise Pascal, the SI unit of pressure is called pascal, denoted as $Pa$.
Let us consider a numerical example to understand the effects of thrust acting on different areas.
Example 9.6 A block of wood is kept on a tabletop. The mass of wooden block is 5 $kg$ and its dimensions are $40 cm \times 20$ $cm \times 10 cm$. Find the pressure exerted
(a)
(b) Fig. 9.4 by the wooden block on the table top if it is made to lie on the table top with its sides of dimensions (a) $20 cm \times 10 cm$ and (b) $40 cm \times 20 cm$.
Solution:
The mass of the wooden block $=5 kg$ The dimensions
$ =40 cm \times 20 cm \times 10 cm $
Here, the weight of the wooden block applies a thrust on the table top.
That is,
$$ \begin{aligned} \text{ Thrust }=F & =m \times g \\ & =5 kg \times 9.8 m s^{-2} \\ & =49 N \end{aligned} $$
Area of a side $=$ length $\times$ breadth
$$ \begin{aligned} & =20 cm \times 10 cm \\ & =200 cm^{2}=0.02 m^{2} \end{aligned} $$
From Eq. (9.20),
$$ \begin{aligned} \text{ Pressure } & =\frac{49 N}{0.02 m^{2}} \\ & =2450 N m^{-2} . \end{aligned} $$
When the block lies on its side of dimensions $40 cm \times 20 cm$, it exerts the same thrust.
Area $=$ length $\times$ breadth
$$ \begin{aligned} & =40 cm \times 20 cm \\ & =800 cm^{2}=0.08 m^{2} \end{aligned} $$
From Eq. (9.20),
$$ \begin{aligned} \text{ Pressure } & =\frac{49 N}{0.08 m^{2}} \\ & =612.5 N m^{-2} \end{aligned} $$
The pressure exerted by the side $20 cm$ $\times 10 cm^{2} 2450 N m^{-2}$ and by the side $40 cm \times 20 cm$ is $612.5 N m^{-2}$.
Thus, the same force acting on a smaller area exerts a larger pressure, and a smaller pressure on a larger area. This is the reason why a nail has a pointed tip, knives have sharp edges and buildings have wide foundations.
9.5.1 PRESSURE IN FLUIDS
All liquids and gases are fluids. A solid exerts pressure on a surface due to its weight. Similarly, fluids have weight, and they also exert pressure on the base and walls of the container in which they are enclosed. Pressure exerted in any confined mass of fluid is transmitted undiminished in all directions.
9.5.2 BUOYANCY
Have you ever had a swim in a pool and felt lighter? Have you ever drawn water from a well and felt that the bucket of water is heavier when it is out of the water? Have you ever wondered why a ship made of iron and steel does not sink in sea water, but while the same amount of iron and steel in the form of a sheet would sink? These questions can be answered by taking buoyancy in consideration. Let us understand the meaning of buoyancy by doing an activity.
Activity 9.4
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Take an empty plastic bottle. Close the mouth of the bottle with an airtight stopper. Put it in a bucket filled with water. You see that the bottle floats.
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Push the bottle into the water. You feel an upward push. Try to push it further down. You will find it difficult to push deeper and deeper. This indicates that water exerts a force on the bottle in the upward direction. The upward force exerted by the water goes on as the bottle is pushed deeper till it is completely immersed.
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Now, release the bottle. It bounces back to the surface.
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Does the force due to the gravitational attraction of the earth act on this bottle? If so, why doesn’t the bottle stay immersed in water after it is released? How can you immerse the bottle in water?
The force due to the gravitational attraction of the earth acts on the bottle in the downward direction. So the bottle is pulled downwards. But the water exerts an upward force on the bottle. Thus, the bottle is pushed upwards. We have learnt that weight of an object is the force due to gravitational attraction of the earth. When the bottle is immersed, the upward force exerted by the water on the bottle is greater than its weight. Therefore it rises up when released.
To keep the bottle completely immersed, the upward force on the bottle due to water must be balanced. This can be achieved by an externally applied force acting downwards. This force must at least be equal to the difference between the upward force and the weight of the bottle.
The upward force exerted by the water on the bottle is known as upthrust or buoyant force. In fact, all objects experience a force of buoyancy when they are immersed in a fluid. The magnitude of this buoyant force depends on the density of the fluid.
9.5.3 WHY OBJECTS FLOAT OR SINK WHEN PLACED ON THE SURFACE OF WATER?
Let us do the following activities to arrive at an answer for the above question.
Activity 9.5
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Take a beaker filled with water.
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Take an iron nail and place it on the surface of the water.
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Observe what happens.
The nail sinks. The force due to the gravitational attraction of the earth on the iron nail pulls it downwards. There is an upthrust of water on the nail, which pushes it upwards. But the downward force acting on the nail is greater than the upthrust of water on the nail. So it sinks (Fig. 9.5).
Fig. 9.5: An iron nail sinks and a cork floats when placed on the surface of water.
Activity 9.6
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Take a beaker filled with water. Take a piece of cork and an iron nail of equal mass.
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Place them on the surface of water.
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Observe what happens.
The cork floats while the nail sinks. This happens because of the difference in their densities. The density of a substance is defined as the mass per unit volume. The density of cork is less than the density of water. This means that the upthrust of water on the cork is greater than the weight of the cork. So it floats (Fig. 9.5).
The density of an iron nail is more than the density of water. This means that the upthrust of water on the iron nail is less than the weight of the nail. So it sinks.
Therefore objects of density less than that of a liquid float on the liquid. The objects of density greater than that of a liquid sink in the liquid.
Questions
1. Why is it difficult to hold a school bag having a strap made of a thin and strong string?
Answer
It is difficult to hold a school bag having a thin strap because the pressure on the shoulders is quite large. This is because the pressure is inversely proportional to the surface area on which the force acts. The smaller is the surface area the larger wold be the pressure on the surface. In the case of a thin strap, the contact surface area is very small. Hence pressure exerted on the shoulder is very large.
2. What do you mean by buoyancy?
Answer
The upward force exerted by a liquid on an object that is immersed in it is known as buoyancy.
3. Why does an object float or sink when placed on the surface of water?
Answer
If the density of an object is more then the density of the liquid then the object would sink this happens because in this case buoyant force that is acting on the object due to liquid is less than the force of gravity acting on the object. If the density of object is less than the density of the liquid, then it floats on the surface of the liquid, this happens because the buoyant force acting on the object is greater than the force of gravity.
9.6 Archimedes’ Principle
Activity 9.7
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Take a piece of stone and tie it to one end of a rubber string or a spring balance.
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Suspend the stone by holding the balance or the string as shown in Fig. 9.6 (a).
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Note the elongation of the string or the reading on the spring balance due to the weight of the stone.
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Now, slowly dip the stone in the water in a container as shown in Fig. 9.6 (b).
(a)
(b) Fig. 9.6: (a) Observe the elongation of the rubber string due to the weight of a piece of stone suspended from it in air. (b) The elongation decreases as the stone is immersed in water.
- Observe what happens to elongation of the string or the reading on the balance.
You will find that the elongation of the string or the reading of the balance decreases as the stone is gradually lowered in the water. However, no further change is observed once the stone gets fully immersed in the water. What do you infer from the decrease in the extension of the string or the reading of the spring balance?
We know that the elongation produced in the string or the spring balance is due to the weight of the stone. Since the extension decreases once the stone is lowered in water, it means that some force acts on the stone in upward direction. As a result, the net force on the string decreases and hence the elongation also decreases. As discussed earlier, this upward force exerted by water is known as the force of buoyancy.
What is the magnitude of the buoyant force experienced by a body? Is it the same in all fluids for a given body? Do all bodies in a given fluid experience the same buoyant force? The answer to these questions is contained in Archimedes’ principle, stated as follows:
When a body is immersed fully or partially in a fluid, it experiences an upward force that is equal to the weight of the fluid displaced by it.
Now, can you explain why a further decrease in the elongation of the string was not observed in activity 9.7, as the stone was fully immersed in water?
Archimedes was a Greek scientist. He discovered the principle, subsequently named
after him, after noticing that the water in a bathtub overflowed when he stepped into it. He ran through the streets shouting “Eureka!”, which means “I have got it”. This knowledge helped him to determine the purity of the Archimedes gold in the crown made for the king.
His work in the field of Geometry and Mechanics made him famous. His understanding of levers, pulleys, wheelsand-axle helped the Greek army in its war with Roman army.
What you have learnt
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The law of gravitation states that the force of attraction between any two objects is proportional to the product of their masses and inversely proportional to the square of the distance between them. The law applies to objects anywhere in the universe. Such a law is said to be universal.
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Gravitation is a weak force unless large masses are involved. The force of gravity decreases with altitude. It also varies on the surface of the earth, decreasing from poles to the equator.
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The weight of a body is the force with which the earth attracts it.
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The weight is equal to the product of mass and acceleration due to gravity.
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The weight may vary from place to place but the mass stays constant. Archimedes’ principle has many applications. It is used in designing ships and submarines. Lactometers, which are used to determine the purity of a sample of milk and hydrometers used for determining density of liquids, are based on this principle.
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All objects experience a force of buoyancy when they are immersed in a fluid.
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Objects having density less than that of the liquid in which they are immersed, float on the surface of the liquid. If the density of the object is more than the density of the liquid in which it is immersed then it sinks in the liquid.
Questions
1. You find your mass to be $42 kg$ on a weighing machine. Is your mass more or less than $42 kg$ ?
Answer
On a weighing machine mass is measured by comparing the weights. So when you weigh your body an upward force (buoyant force) acts on it which causes machine to show your weight less than the actual weight.
2. You have a bag of cotton and an iron bar, each indicating a mass of $100 kg$ when measured on a weighing machine. In reality, one is heavier than other. Can you say which one is heavier and why?
Answer
Actual weight of any object is equal to the sum of its measured weight and the buoyant force. The bag of cotton is heavier since it is larger than iron bar, so the buoyant force is larger in case of cotton henceactual weight of cotton bag is more and it is heavier.
Exercises
1. How does the force of gravitation between two objects change when the distance between them is reduced to half?
Answer
Consider the Universal law of gravitation,
According to that law, the force of attraction between two bodies is
$\mathrm{F} =\frac{(\mathrm{Gm_1m_2})}{r^2}$
Where,
$\mathrm{m_1}$ and $\mathrm{m2}$ are the masses of the two bodies.
$\mathrm{G}$ is the gravitational constant.
$\mathrm{r}$ is the distance between the two bodies.
Given that the distance is reduced to half then,
$\mathrm{r}= 1/2 ~r$
$\mathrm{F} =\frac{(\mathrm{Gm_1m_2})}{r^2}$
$\mathrm{F} =\frac{(\mathrm{Gm_1m_2})}{(\frac{r}{2})^2}$
$\mathrm{F} =\frac{4(\mathrm{Gm_1m_2})}{r^2}$
$\mathrm{F} = 4\mathrm{F}$
Therefore once the space between the objects is reduced to half, then the force of gravitation will increase by fourfold the first force.
2. Gravitational force acts on all objects in proportion to their masses. Why then, a heavy object does not fall faster than a light object?
Answer
All objects fall from the top with a constant acceleration called acceleration due to gravity (g). This is constant on earth and therefore the value of ‘g’ doesn’t depend on the mass of an object. Hence, heavier objects don’t fall quicker than light-weight objects provided there’s no air resistance.
3. What is the magnitude of the gravitational force between the earth and a $1 kg$ object on its surface? (Mass of the earth is $6 \times 10^{24} kg$ and radius of the earth is $6.4 \times 10^{6} m$.)
Answer
From Newton’s law of gravitation, we know that the force of attraction between the bodies is given by
$$ F=\frac{\left(G m_1 m_2\right)}{r^2} $$
Here
$ \begin{aligned} & m_1=\text { mass of Earth }=6.0 \times 10^{24} \mathrm{~kg} \\ & m_2=\text { mass of the body }=1 \mathrm{~kg} \end{aligned} $
$r=$ distance between the two bodies
Radius of Earth $=6.4 \times 10^6 \mathrm{~m}$
$\mathrm{G}=$ Universal gravitational constant $=6.67 \times 10^{-11} \mathrm{Nm}^2 \mathrm{~kg}^{-2}$
By substituting all the values in the equation
$$ \begin{aligned} & F=\frac{\left(G m_1 m_2\right)}{r^2} \\ & F=\frac{6.67 \times 10^{-11}\left(6.0 \times 10^{24} \times 1\right)}{\left(6.4 \times 10^6\right)^2} \\ & \mathrm{~F}=9.8 \mathrm{~N} \\ \end{aligned} $$
This shows that Earth exerts a force of $9.8 \mathrm{~N}$ on a body of mass $1 \mathrm{~kg}$. The body will exert an equal force of attraction of $9.8 \mathrm{~N}$ on the Earth.
4. The earth and the moon are attracted to each other by gravitational force. Does the earth attract the moon with a force that is greater or smaller or the same as the force with which the moon attracts the earth? Why?
Answer
The earth attracts the moon with a force same as the force with which the moon attracts the earth. However, these forces are in opposite directions. By universal law of gravitation, the force between moon and also the sun can be
$$ F=\frac{\left(G m_1 m_2\right)}{d^2} $$
Where,
$\mathrm{d}=$ distance between the earth and moon.
$\mathrm{m}_1$ and $\mathrm{m}_2=$ masses of earth and moon respectively.
5. If the moon attracts the earth, why does the earth not move towards the moon?
Answer
According to the universal law of gravitation and Newton’s third law, we all know that the force of attraction between two objects is the same, however in the opposite directions. So the earth attracts the moon with a force same as the moon attracts the earth but in opposite directions. Since earth is larger in mass compared to that of the moon, it accelerates at a rate lesser than the acceleration rate of the moon towards the Earth. Therefore, for this reason the earth does not move towards the moon.
6. What happens to the force between two objects, if
(i) the mass of one object is doubled?
(ii) the distance between the objects is doubled and tripled?
(iii) the masses of both objects are doubled?
Answer
(i)
According to universal law of gravitation, the force between 2 objects $\left(\mathrm{m}_1\right.$ and $\left.\mathrm{m}_2\right)$ is proportional to their plenty and reciprocally proportional to the sq. of the distance(R) between them.
$$ F=\frac{\left(G 2 m_1 m_2\right)}{R^2} $$
If the mass is doubled for one object.
$\mathrm{F}=2 \mathrm{~F}$, so the force is also doubled.
(ii)
If the distance between the objects is doubled and tripled
If it’s doubled
Hence,
$ \begin{aligned} & \mathrm{F}=\left(\mathrm{Gm}_1 \mathrm{~m}_2\right) /(2 \mathrm{R})^2 \\ & \mathrm{~F}=1 / 4\left(\mathrm{Gm}_1 \mathrm{~m}_2\right) / \mathrm{R}^2 \\ & \mathrm{~F}=\mathrm{F} / 4 \end{aligned} $
Force thus becomes one-fourth of its initial force.
Now, if it’s tripled
Hence,
$ \begin{aligned} & \mathrm{F}=\left(\mathrm{Gm}_1 \mathrm{~m}_2\right) /(3 \mathrm{R})^2 \\ & \mathrm{~F}=1 / 9\left(\mathrm{Gm}_1 \mathrm{~m}_2\right) / \mathrm{R}^2 \\ & \mathrm{~F}=\mathrm{F} / 9 \end{aligned} $
Force thus becomes one-ninth of its initial force.
(iii)
If masses of both the objects are doubled, then
$ F=\frac{\left(G 2 m_1 2 m_2\right)}{R^2} $
$F=4 F$, Force will therefore be four times greater than its actual value.
7. What is the importance of universal law of gravitation?
Answer
The universal law of gravitation explains many phenomena that were believed to be unconnected:
(i) The motion of the moon round the earth
(ii) The responsibility of gravity on the weight of the body which keeps us on the ground
(iii) The tides because of the moon and therefore the Sun
(iv) The motion of planets round the Sun
8. What is the acceleration of free fall?
Answer
Acceleration due to gravity is the acceleration gained by an object due to gravitational force. On Earth, all bodies experience a downward force of gravity which Earth’s mass exerts on them. The Earth’s gravity is measured by the acceleration of the freely falling objects. At Earth’s surface, the acceleration of gravity is $9.8 \mathrm{~ms}^{-2}$ and it is denoted by ’ $\mathrm{g}$ ‘. Thus, for every second an object is in free fall, its speed increases by about 9.8 metres per second.
9. What do we call the gravitational force between the earth and an object?
Answer
The gravitation force between the earth and an object is called weight. Weight is equal to the product of acceleration due to the gravity and mass of the object.
10. Amit buys few grams of gold at the poles as per the instruction of one of his friends. He hands over the same when he meets him at the equator. Will the friend agree with the weight of gold bought? If not, why? [Hint: The value of $g$ is greater at the poles than at the equator.]
Answer
The weight of a body on the earth’s surface;
W = mg (where m = mass of the body and g = acceleration due to gravity)
The value of g is larger at poles when compared to the equator. So gold can weigh less at the equator as compared to the poles.
Therefore, Amit’s friend won’t believe the load of the gold bought.
11. Why will a sheet of paper fall slower than one that is crumpled into a ball?
Answer
A sheet of paper has a larger surface area when compared to a crumpled paper ball. A sheet of paper will face a lot of air resistance. Thus, a sheet of paper falls slower than the crumpled ball.
12. Gravitational force on the surface of the moon is only $\frac{1}{6}$ as strong as gravitational force on the earth. What is the weight in newtons of a $10 kg$ object on the moon and on the earth?
Answer
Given data:
Acceleration due to earth’s gravity $=\mathrm{g}_{\mathrm{c}}$ or $\mathrm{g}=9.8 \mathrm{~m} / \mathrm{s}^2$
Object’s mass, $\mathrm{m}=10 \mathrm{~kg}$
Acceleration due to moon gravity $=\mathrm{g}_{\mathrm{m}}$
Weight on the earth $=\mathrm{W}_{\mathrm{c}}$
Weight on the moon $=\mathrm{W}_{\mathrm{m}}$
Weight $=$ mass $\times$ gravity
$\mathrm{g_m}=(1 / 6) \mathrm{g_c}$ (given)
So $\mathrm{W_m}=\mathrm{mg_m}=\mathrm{mx}(1 / 6) \mathrm{g_c}$
$\mathrm{W}_{\mathrm{m}}=10 \times(1 / 6) \times 9.8=16.34 \mathrm{~N}$
$\mathrm{W_c}=\mathrm{m} \mathrm{x} \mathrm{g_c}=10 \times 9.8$
$\mathrm{W}_{\mathrm{e}}=98 \mathrm{~N}$
13. A ball is thrown vertically upwards with a velocity of $49 m / s$. Calculate
(i) the maximum height to which it rises,
(ii) the total time it takes to return to the surface of the earth.
Answer
Given data:
Initial velocity $\mathrm{u}=49 \mathrm{~m} / \mathrm{s}$
Final speed $\mathrm{v}$ at maximum height $=0$
Acceleration due to earth gravity $\mathrm{g}=-9.8 \mathrm{~m} / \mathrm{s}^2$ (thus negative as ball is thrown up).
By third equation of motion,
$ \begin{aligned} & 2 \mathrm{gH}=\mathrm{v}^2-\mathrm{u}^2 \\ & 2 \times(-9.8) \times \mathrm{H}=0-(49)^2 \\ & -19.6 \mathrm{H}=-2401 \\ & \mathrm{H}=122.5 \mathrm{~m} \end{aligned} $
Total time $\mathrm{T}=$ Time to ascend $\left(\mathrm{T_a}\right)+$ Time to descend $\left(\mathrm{T_d} \right)$
$ \begin{aligned} & \mathrm{v}=\mathrm{u}+\mathrm{gt} \\ & 0=49+(-9.8) \times \mathrm{T}_{\mathrm{a}} \\ & \mathrm{Ta}=(49 / 9.8)=5 \mathrm{~s} \end{aligned} $
Also, $\mathrm{T}_{\mathrm{d}}=5 \mathrm{~s}$
Therefore $\mathrm{T}=\mathrm{T_a} +\mathrm{T_d}$
$ \begin{aligned} & \mathrm{T}=5+5 \\ & \mathrm{~T}=10 \mathrm{~s} \end{aligned} $
14. A stone is released from the top of a tower of height $19.6 m$. Calculate its final velocity just before touching the ground.
Answer
Given data:
Initial velocity
$ \mathrm{u}=0 $
Tower height $=$ total distance $=19.6 \mathrm{~m}$
$ \mathrm{g}=9.8 \mathrm{~m} / \mathrm{s}^2 $
Consider third equation of motion
$ \begin{aligned} & \mathrm{v}^2=\mathrm{u}^2+2 \mathrm{gs} \\ & \mathrm{v}^2=0+2 \times 9.8 \times 19.6 \\ & \mathrm{v}^2=384.16 \\ & \mathrm{v}=\sqrt{ }(384.16) \\ & \mathrm{v}=19.6 \mathrm{~m} / \mathrm{s} \end{aligned} $
15. A stone is thrown vertically upward with an initial velocity of $40 m / s$. Taking $g=10 m / s^{2}$, find the maximum height reached by the stone. What is the net displacement and the total distance covered by the stone?
Answer
Given data:
Initial velocity $u=40 \mathrm{~m} / \mathrm{s}$
$ \mathrm{g}=10 \mathrm{~m} / \mathrm{s}^2 $
Max height final velocity $=0$
Consider third equation of motion
$\mathrm{v}^2=\mathrm{u}^2-2 \mathrm{gs}$ [negative as the object goes up]
$ \begin{aligned} & 0=(40)^2-2 \times 10 \times s \\ & \mathrm{~s}=(40 \times 40) / 20 \end{aligned} $
Maximum height $\mathrm{s}=80 \mathrm{~m}$
Total Distance $=\mathrm{s}+\mathrm{s}=80+80$
Total Distance $=160 \mathrm{~m}$
Total displacement $=0$ (The first point is the same as the last point)
16. Calculate the force of gravitation between the earth and the Sun, given that the mass of the earth $=6 \times 10^{24} kg$ and of the Sun $=2 \times 10^{30} kg$. The average distance between the two is $1.5 \times 10^{11} m$.
Answer
Given data:
Mass of the sun $\mathrm{m}_{\mathrm{s}}=2 \times 10^{30} \mathrm{~kg}$
Mass of the earth $\mathrm{m}_{\mathrm{c}}=6 \times 10^{24} \mathrm{~kg}$
Gravitation constant $\mathrm{G}=6.67 \times 10^{-11} \mathrm{~N} \mathrm{~m}^2 / \mathrm{kg}^2$
Average distance $\mathrm{r}=1.5 \times 10^{11} \mathrm{~m}$
Consider Universal law of Gravitation
$ \begin{aligned} & F=\frac{\left(G m_1 m_2\right)}{d^2} \\ & F=\frac{\left(6.67 \times 10^{-11} \times 6 \times 10^{24} \times 2 \times 10^{30}\right)}{\left(1.5 \times 10^{11}\right)^2} \\ & \mathrm{~F}=3.56 \times 10^{22} \mathrm{~N} \end{aligned} $
17. A stone is allowed to fall from the top of a tower $100 m$ high and at the same time another stone is projected vertically upwards from the ground with a velocity of $25 m / s$. Calculate when and where the two stones will meet.
Answer
Given data:
(i) When the stone from the top of the tower is thrown, Initial velocity $u^{\prime}=0$
Distance travelled $=\mathrm{x}$
Time taken $=\mathrm{t}$
Therefore,
$ \begin{aligned} & s=u t+\frac{1}{2} g t^2 \\ & x=0+(1 / 2) g^2 \\ & x=5 t^2—–(a) \end{aligned} $
(ii) When the stone is thrown upwards,
Initial velocity $u=25 \mathrm{~m} / \mathrm{s}$
Distance travelled $=(100-\mathrm{x})$
Time taken $=\mathrm{t}$
$ \begin{aligned} & s=u t-\frac{1}{2} g t^2 \\ & (100-\mathrm{x})=25 \mathrm{t}-(1 / 2) \times 10 \mathrm{xt}^2 \\ & \mathrm{x}=100-25 \mathrm{t}+5 \mathrm{t}^2—– \text { (b) } \end{aligned} $
From equations (a) and (b)
$ \begin{aligned} & 5 \mathrm{t}^2=100-25 \mathrm{t}+5 \mathrm{t}^2 \\ & \mathrm{t}=(100 / 25)=4 \mathrm{sec} . \end{aligned} $
After 4sec, two stones will meet
From (a)
$ \mathrm{x}=5 \mathrm{t}^2=5 \mathrm{x} 4 \times 4=80 \mathrm{~m} . $
Putting the value of $x$ in (100-x)
$ =(100-80)=20 \mathrm{~m} \text {. } $
This means that after $4 \mathrm{sec}, 2$ stones meet a distance of $20 \mathrm{~m}$ from the ground.
18. A ball thrown up vertically returns to the thrower after $6 s$. Find
(a) the velocity with which it was thrown up,
(b) the maximum height it reaches, and
(c) its position after $4 s$.
Answer
Given data:
$ \mathrm{g}=10 \mathrm{~m} / \mathrm{s}^2 $
Total time $\mathrm{T}=6 \mathrm{sec}$
$ \mathrm{T_a}=\mathrm{T_d}=3 \mathrm{sec} $ (a) Final velocity at maximum height $\mathrm{v}=0$
From first equation of motion:-
$ \begin{aligned} & \mathrm{v}=\mathrm{u}-\mathrm{gt_a} \\ & \mathrm{u}=\mathrm{v}+\mathrm{gt_a} \\ & =0+10 \times 3 \\ & =30 \mathrm{~m} / \mathrm{s} \end{aligned} $
The velocity with which stone was thrown up is $30 \mathrm{~m} / \mathrm{s}$.
(b) From second equation of motion
$ \begin{aligned} & s=u t_a-\frac{1}{2} g\left(t_a\right)^2 \\ & =30 \times 3-(1 / 2) \times 10 \times(3)^2 \\ & =90-45=45 \mathrm{~m} \end{aligned} $
The maximum height stone reaches is $45 \mathrm{~m}$.
(c) In $3 \mathrm{sec}$, it reaches the maximum height.
Distance travelled in another $1 \mathrm{sec}=\mathrm{s}$,
$ \begin{aligned} & s=u t_a-\frac{1}{2} g\left(t_a\right)^2 \\ & \mathrm{~s}=0+10 \times 1 \times 1 \\ & \mathrm{~s}=5 \mathrm{~m} . \end{aligned} $
The distance travelled in another $1 \mathrm{sec}=5 \mathrm{~m}$.
Therefore in $4 \mathrm{sec}$, the position of point $\mathrm{p}(45-5)$ $=40 \mathrm{~m}$ from the ground.
19. In what direction does the buoyant force on an object immersed in a liquid act?
Answer
The buoyant force on an object that is immersed in a liquid will be in a vertically upward direction.
20. Why does a block of plastic released under water come up to the surface of water?
Answer
The density of plastic is lesser than that of water. Therefore, the force of buoyancy on plastic block will be greater than the weight of plastic block. Hence, the acceleration of plastic block is going to be in the upward direction. So, the plastic block comes up to the surface of water.
21. The volume of $50 g$ of a substance is $20 cm^{3}$. If the density of water is $1 g cm^{-3}$, will the substance float or sink?
Answer
To find the Density of the substance the formula is
Density $=($ Mass/Volume $)$
Density $=(50 / 20)=2.5 \mathrm{~g} / \mathrm{cm}^3$
Density of water $=1 \mathrm{~g} / \mathrm{cm}^3$
Density of the substance is greater than density of water. So the substance will sink.
22. The volume of a $500 g$ sealed packet is $350 cm^{3}$. Will the packet float or sink in water if the density of water is $1 g$ $cm^{-3}$ ? What will be the mass of the water displaced by this packet?
Answer
Density of sealed packet $=500 / 350=1.42 \mathrm{~g} / \mathrm{cm}^3$
Density of sealed packet is greater than density of water
Therefore the packet will sink.
Considering Archimedes Principle,
Displaced water volume $=$ Force exerted on the sealed packet.
Volume of water displaced $=350 \mathrm{~cm}^3$
Therefore displaced water mass $=\rho \times \mathrm{V}$
$ =1 \times 350 $
Mass of displaced water $=350 \mathrm{~g}$.