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Just as precise measurements are necessary in science, it is equally important to be able to make rough estimates of quantities using rudimentary ideas and common observations. Think of ways by which you can estimate the following (where an estimate is difficult to obtain, try to get an upper bound on the quantity):
(a) the total mass of rain-bearing clouds over India during the Monsoon
(b) the mass of an elephant
(c) the wind speed during a storm
(d) the number of strands of hair on your head
(e) the number of air molecules in your classroom .
(a) the total mass of rain-bearing clouds over India during the Monsoon
(b) the mass of an elephant
(c) the wind speed during a storm
(d) the number of strands of hair on your head
(e) the number of air molecules in your classroom .
Solution:
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(a) The average rainfall of nearly $100 \mathrm{~cm}$ or $1 \mathrm{~m}$ is recorded by meteorologists, during Monsoon, in India. If $\mathrm{A}$ is the area of the country, then $\mathrm{A}=3.3$ million sq. $\mathrm{km}=3.3 \times 10^6(\mathrm{~km})^2$ $=3.3 \times 10^6 \times 10^6 \mathrm{~m}^2=3.3 \times 10^{12} \mathrm{~m}^2$
Mass of rain - bearing clouds
$=$ Volume of rain water $\times$ density of water $=3.3 \times 10^{12} \mathrm{~m}^2 \times 1 \mathrm{~m} \times 1000 \mathrm{~kg} / \mathrm{m}^3$ $=3.3 \times 10^{15} \mathrm{~kg}$.
(b) Measure the depth of an empty boat in water. Let it be $d_1$. If $A$ be the base area the boat, then volume of water displaced by boat, $V_1=A \mathrm{~d}_1$.
Let $d_2$ be the depth of boat in water when the elephant is moved into the boat. Volume of water displaced by (boat $+$ elephant), $V_2=A d_2$
Volume of water displaced by elephant,
$$
V=V_2-V_1=A\left(d_2-d_1\right)
$$
If $\rho$ be the density of water, then mass of elephant $=$ mass of water displaced by it $=A\left(d_2-d_1\right) \rho$.
(c) Wind speed during storms can be estimated by floating a gas-filled balloon in air at a known height $h$. When there is no wind, the balloon is at $\mathrm{A}$. Suppose the wind starts blowing to the right such that the balloon reaches position B in 1 second. Now, $A B=d=h \theta$.

The value of directly gives the wind speed.
(d) Let us assume that the hair on our head are uniformly distributed. Thickness of a human hair is $5 \times 10^{-5} \mathrm{~m}$.
Number of hair on the head
$=\frac{\text { area of the head }}{\text { area of cross-section of a hair }}$
Taking head to be a circle of radius $8 \mathrm{~cm}$, number of hair on head
$$
=\frac{\pi(0.08)^2}{\pi\left(5 \times 10^{-5}\right)^2}=\frac{64 \times 10^{-4}}{25 \times 10^{-10}}=2.56 \times 10^6
$$
The number of hair on the human head is of the order of one million.
(e) Consider a class room of size $10 \mathrm{~m} \times 8 \mathrm{~m} \times 4 \mathrm{~m}$. Volume of this room is $320 \mathrm{~m}^3$. We know that $22.4 \mathrm{~L}$ or $22.4 \times 10^{-3} \mathrm{~m}^3$ of air has $6.02 \times 10^{23}$ molecules (equal to' Avogadro's number).
$\therefore \quad$ Number of molecules of air in the class room
$$
=\frac{6.02 \times 10^{23}}{22.4 \times 10^{-3}} \times 320=8.6 \times 10^{27}
$$
Mass of rain - bearing clouds
$=$ Volume of rain water $\times$ density of water $=3.3 \times 10^{12} \mathrm{~m}^2 \times 1 \mathrm{~m} \times 1000 \mathrm{~kg} / \mathrm{m}^3$ $=3.3 \times 10^{15} \mathrm{~kg}$.
(b) Measure the depth of an empty boat in water. Let it be $d_1$. If $A$ be the base area the boat, then volume of water displaced by boat, $V_1=A \mathrm{~d}_1$.
Let $d_2$ be the depth of boat in water when the elephant is moved into the boat. Volume of water displaced by (boat $+$ elephant), $V_2=A d_2$
Volume of water displaced by elephant,
$$
V=V_2-V_1=A\left(d_2-d_1\right)
$$
If $\rho$ be the density of water, then mass of elephant $=$ mass of water displaced by it $=A\left(d_2-d_1\right) \rho$.
(c) Wind speed during storms can be estimated by floating a gas-filled balloon in air at a known height $h$. When there is no wind, the balloon is at $\mathrm{A}$. Suppose the wind starts blowing to the right such that the balloon reaches position B in 1 second. Now, $A B=d=h \theta$.

The value of directly gives the wind speed.
(d) Let us assume that the hair on our head are uniformly distributed. Thickness of a human hair is $5 \times 10^{-5} \mathrm{~m}$.
Number of hair on the head
$=\frac{\text { area of the head }}{\text { area of cross-section of a hair }}$
Taking head to be a circle of radius $8 \mathrm{~cm}$, number of hair on head
$$
=\frac{\pi(0.08)^2}{\pi\left(5 \times 10^{-5}\right)^2}=\frac{64 \times 10^{-4}}{25 \times 10^{-10}}=2.56 \times 10^6
$$
The number of hair on the human head is of the order of one million.
(e) Consider a class room of size $10 \mathrm{~m} \times 8 \mathrm{~m} \times 4 \mathrm{~m}$. Volume of this room is $320 \mathrm{~m}^3$. We know that $22.4 \mathrm{~L}$ or $22.4 \times 10^{-3} \mathrm{~m}^3$ of air has $6.02 \times 10^{23}$ molecules (equal to' Avogadro's number).
$\therefore \quad$ Number of molecules of air in the class room
$$
=\frac{6.02 \times 10^{23}}{22.4 \times 10^{-3}} \times 320=8.6 \times 10^{27}
$$
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