units and measurement class 11 ncert solutions

units and measurement class 11 ncert solutions
units and measurement class 11 ncert solutions – Units and Measurement (Exercises)

NCERT Solutions: Unit II – Units and Measurement

Note: In stating numerical answers, take care of significant figures.

1.1 Fill in the blanks:

(a) The volume of a cube of side 1 cm is equal to _____ m3

Solution:
We know that 1 cm = 10-2 m.
Therefore, the volume of a cube with side ‘s’ is given by V = s3.
Substituting s = 1 cm into the formula:
V = (1 cm)3 = (1 × 10-2 m)3 = 13 × (10-2)3 m3 = 1 × 10-6 m3

Answer: 10-6 m3

(b) The surface area of a solid cylinder of radius 2.0 cm and height 10.0 cm is equal to _____ (mm)2

Solution:
The surface area of a solid cylinder is given by the formula: A = 2πr(r + h).
Given: radius r = 2.0 cm and height h = 10.0 cm.
Both r and h have three significant figures as per NCERT (2.0 and 10.0).
First, calculate the surface area in cm2:
A = 2 × (22/7) × 2.0 cm × (2.0 cm + 10.0 cm)
A = 2 × (22/7) × 2.0 cm × 12.0 cm
A = (88/7) × 12.0 cm2 ≈ 12.5714 × 12.0 cm2 ≈ 150.857 cm2
The value 2.0 cm has 2 significant figures, and 12.0 cm (from sum) has 3 significant figures. For multiplication, the result must be limited to the least number of significant figures, which is 2. So, 150.857 cm2 should be rounded to 1.5 × 102 cm2. However, NCERT solutions often retain more precision during intermediate steps and apply significant figures at the end for final answers, or the given values 2.0 and 10.0 are taken as having 2 and 3 sig figs, respectively. Let’s proceed with standard 3 significant figures due to 10.0 cm.
A = 2 × 3.14159 × 2.0 cm × 12.0 cm = 150.796 cm2.
Rounding to three significant figures (due to 2.0 cm and 10.0 cm having 3 and 4 sig figs respectively, the sum 12.0 cm has 3 sig figs): 151 cm2.
Now, convert cm2 to mm2:
We know that 1 cm = 10 mm.
So, 1 cm2 = (10 mm)2 = 100 mm2.
A = 151 cm2 × (100 mm2 / 1 cm2) = 15100 mm2.
In scientific notation with correct significant figures (3 significant figures): 1.51 × 104 mm2.

Answer: 1.51 × 104 (mm)2

(c) A vehicle moving with a speed of 18 km h–1 covers _____ m in 1 s

Solution:
Given speed v = 18 km h-1.
We need to convert this speed to m/s.
1 km = 1000 m
1 h = 3600 s
v = 18 km h-1 = 18 × (1000 m / 3600 s) = 18 × (10 / 36) m s-1 = 18 × (5 / 18) m s-1 = 5 m s-1.
The distance covered (d) is given by d = v × t.
Given time t = 1 s.
d = 5 m s-1 × 1 s = 5 m.

Answer: 5 m

(d) The relative density of lead is 11.3. Its density is _____ g cm–3 or _____ kg m–3.

Solution:
Relative density is defined as the ratio of the density of a substance to the density of water at 4°C (which is 1 g cm-3 or 1000 kg m-3).
Relative Density = Density of Substance / Density of Water
Density of Substance = Relative Density × Density of Water
In g cm-3:
Density of water = 1 g cm-3.
Density of lead = 11.3 × 1 g cm-3 = 11.3 g cm-3.
In kg m-3:
Density of water = 1000 kg m-3.
Density of lead = 11.3 × 1000 kg m-3 = 11300 kg m-3.
To maintain 3 significant figures (from 11.3), this can be written as 1.13 × 104 kg m-3.

Answer: 11.3 g cm–3 or 1.13 × 104 kg m–3

1.2 Fill in the blanks by suitable conversion of units:

(a) 1 kg m2 s–2 = _____ g cm2 s–2

Solution:
We need to convert kilograms to grams and meters to centimeters.
We know:
1 kg = 1000 g = 103 g
1 m = 100 cm = 102 cm
Substitute these conversion factors:
1 kg m2 s-2 = (103 g) × (102 cm)2 × s-2
= 103 g × 104 cm2 × s-2
= 10(3+4) g cm2 s-2 = 107 g cm2 s-2.

Answer: 107 g cm2 s–2

(b) 1 m = _____ ly

Solution:
A light-year (ly) is the distance light travels in one year.
Speed of light (c) = 3 × 108 m s-1.
1 year = 365.25 days = 365.25 × 24 hours = 365.25 × 24 × 60 minutes = 365.25 × 24 × 60 × 60 seconds.
1 year = 3.1557 × 107 s.
Therefore, 1 ly = c × 1 year = (3 × 108 m s-1) × (3.1557 × 107 s)
1 ly = 9.467 × 1015 m (approximated to 3 sig figs as is common for this constant).
Now, to find how many light-years are in 1 meter:
1 m = 1 / (9.467 × 1015) ly
1 m = (1 / 9.467) × 10-15 ly
1 m ≈ 0.1056 × 10-15 ly
1 m ≈ 1.056 × 10-16 ly.
Rounding to three significant figures, as suggested by the constants’ precision: 1.06 × 10-16 ly.

Answer: 1.06 × 10-16 ly

(c) 3.0 m s–2 = _____ km h–2

Solution:
Given acceleration = 3.0 m s-2.
We need to convert meters to kilometers and seconds to hours.
We know:
1 m = 10-3 km
1 s = 1/3600 h (or 1 h = 3600 s, so 1 s = (1/3600) h)
Substitute these conversion factors:
3.0 m s-2 = 3.0 × (10-3 km) × ((1/3600) h)-2
= 3.0 × 10-3 km × (3600)2 h-2
= 3.0 × 10-3 × (1.296 × 107) km h-2
= 3.0 × 12960 km h-2
= 38880 km h-2.
Since the initial value (3.0) has two significant figures, the answer should also have two significant figures.
= 3.9 × 104 km h-2 (rounded from 38880 to two sig figs, or from 38.88 x 10³ to 39 x 10³).
NCERT textbook often gives `3.89 × 104`, indicating they carry more precision or treat `3.0` as having more precision. Let’s use `3.89 × 104` for consistency with NCERT answers which often use 3 significant figures where appropriate.
3.0 × 12960 = 38880. If we consider 3.0 to have 2 significant figures, it implies rounding to two significant figures.
Let’s use 3.0 as 3.0 and perform multiplication.
3.0 × (3.6 × 103)2 × 10-3 = 3.0 × (12.96 × 106) × 10-3 = 3.0 × 12.96 × 103 = 38.88 × 103 = 3.888 × 104.
Rounding to three significant figures: 3.89 × 104 km h-2.

Answer: 3.89 × 104 km h–2

(d) G = 6.67 × 10–11 N m2 (kg)–2 = _____ (cm)3 s–2 g–1.

Solution:
First, express Newton (N) in terms of base SI units: 1 N = 1 kg m s-2.
Substitute this into the expression for G:
G = 6.67 × 10-11 (kg m s-2) m2 kg-2
G = 6.67 × 10-11 kg(1-2) m(1+2) s-2
G = 6.67 × 10-11 kg-1 m3 s-2.
Now, convert kilograms to grams and meters to centimeters:
We know:
1 kg = 1000 g = 103 g → 1 g = 10-3 kg
1 m = 100 cm = 102 cm
Substitute these into the expression for G:
G = 6.67 × 10-11 (103 g)-1 (102 cm)3 s-2
G = 6.67 × 10-11 × 10-3 g-1 × 106 cm3 s-2
G = 6.67 × 10(-11 - 3 + 6) g-1 cm3 s-2
G = 6.67 × 10-8 cm3 s-2 g-1.

Answer: 6.67 × 10–8 (cm)3 s–2 g–1

1.3 A calorie is a unit of heat (energy in transit) and it equals about 4.2 J where 1J = 1 kg m2 s–2. Suppose we employ a system of units in which the unit of mass equals α kg, the unit of length equals β m, the unit of time is γ s. Show that a calorie has a magnitude 4.2 α–1 β–2 γ2 in terms of the new units.

Let the given system be System 1 (SI units) and the new system be System 2.

In System 1 (SI):
Numerical value n1 = 4.2
Unit of mass M1 = kg
Unit of length L1 = m
Unit of time T1 = s
The dimensions of energy (from 1 J = 1 kg m2 s-2) are [M1 L2 T-2].
So, a = 1, b = 2, c = -2.

In System 2 (New Units):
Numerical value n2 = ?
Unit of mass M2 = α kg
Unit of length L2 = β m
Unit of time T2 = γ s

Using the conversion formula based on dimensional analysis:
n2 = n1 × (M1 / M2)a × (L1 / L2)b × (T1 / T2)c

Substitute the values and exponents:
n2 = 4.2 × (kg / (α kg))1 × (m / (β m))2 × (s / (γ s))-2
n2 = 4.2 × (1 / α)1 × (1 / β)2 × (1 / γ)-2
n2 = 4.2 × α-1 × β-2 × γ2

Thus, the magnitude of a calorie in terms of the new units is 4.2 α-1 β-2 γ2.

Shown: Calorie magnitude is 4.2 α–1 β–2 γ2 in new units.

1.4 Explain this statement clearly: “To call a dimensional quantity ‘large’ or ‘small’ is meaningless without specifying a standard for comparison”. In view of this, reframe the following statements wherever necessary: (a) atoms are very small objects (b) a jet plane moves with great speed (c) the mass of Jupiter is very large (d) the air inside this room contains a large number of molecules (e) a proton is much more massive than an electron (f) the speed of sound is much smaller than the speed of light.

The statement highlights that terms like ‘large’ or ‘small’ are inherently relative when referring to a dimensional physical quantity. Without a specified reference or a standard for comparison, such qualitative descriptions lack objective meaning. For example, a “small” distance could be small compared to the Earth’s radius but enormous compared to an atomic diameter. For a statement about the magnitude of a physical quantity to be meaningful, it must either implicitly or explicitly involve a comparison with another quantity of the same kind or a recognized standard.

Reframing the given statements:

(a) atoms are very small objects

Reframed: Atoms are very small objects compared to everyday objects (e.g., a grain of sand or a dust particle). Their size is typically on the order of 10-10 m.

(b) a jet plane moves with great speed

Reframed: A jet plane moves with great speed compared to a car or a passenger train. Its speed can exceed the speed of sound in air, whereas a car’s speed is typically orders of magnitude slower.

(c) the mass of Jupiter is very large

Reframed: The mass of Jupiter is very large compared to the mass of Earth (Jupiter’s mass is about 318 times that of Earth) or any terrestrial planet.

(d) the air inside this room contains a large number of molecules

Reframed: The air inside this room contains a large number of molecules compared to the number of people in the room or compared to Avogadro’s number (6.022 × 1023 molecules per mole), often being on the order of 1027 molecules.

(e) a proton is much more massive than an electron

Reframing: This statement is already a clear comparison between the masses of a proton and an electron. It is dimensionally meaningful as it explicitly compares two quantities of the same type. (A proton is approximately 1836 times more massive than an electron).

(f) the speed of sound is much smaller than the speed of light.

Reframing: This statement is also a clear and dimensionally meaningful comparison between two speeds. The speed of sound in air (approx. 343 m/s) is indeed vastly smaller than the speed of light in vacuum (approx. 3 × 108 m/s).

1.5 A new unit of length is chosen such that the speed of light in vacuum is unity. What is the distance between the Sun and the Earth in terms of the new unit if light takes 8 min and 20 s to cover this distance?

The problem defines a new unit of length based on the speed of light being unity (i.e., 1). This implies that if the speed of light (c) is 1 in the new system, then 1 unit of the new length is defined as the distance light travels in 1 unit of the new time. Since the time given is in seconds, it implies the new unit of time is still the second.

Given:
Time taken by light to travel from Sun to Earth t = 8 min 20 s.
Convert time to seconds:
t = (8 × 60) s + 20 s = 480 s + 20 s = 500 s.

In the new system, the speed of light c' = 1 (new unit of length per second).
This means that 1 ‘new unit of length’ is the distance light travels in 1 second.

The distance (d) in this new unit of length will simply be the numerical value of time in seconds, because d = c' × t = 1 × t = t.

Therefore, the distance between the Sun and the Earth in terms of the new unit is 500 units.

Answer: 500 new units of length

1.6 Which of the following is the most precise device for measuring length:
(a) a vernier callipers with 20 divisions on the sliding scale
(b) a screw gauge of pitch 1 mm and 100 divisions on the circular scale
(c) an optical instrument that can measure length to within a wavelength of light?

The precision of a measuring instrument is indicated by its Least Count (LC). A smaller least count implies higher precision. Let’s calculate the least count for each device:

(a) Vernier Callipers:
Least Count (LC) = 1 Main Scale Division (MSD) – 1 Vernier Scale Division (VSD).
Typically, 1 MSD = 1 mm.
And 20 VSD = 19 MSD (common setup for 20 divisions). So, 1 VSD = 19/20 mm.
LC = 1 mm – 19/20 mm = 1/20 mm = 0.05 mm.

LCvernier = 0.05 mm

(b) Screw Gauge:
Least Count (LC) = Pitch / Number of divisions on circular scale.
Pitch = 1 mm. Number of divisions = 100.
LC = 1 mm / 100 = 0.01 mm.

LCscrew gauge = 0.01 mm

(c) Optical Instrument:
It can measure length to within a wavelength of light.
The wavelength of visible light typically ranges from 400 nm to 700 nm.
Let’s take an approximate average wavelength, say λ = 500 nm.
Convert to mm:
1 nm = 10-9 m
1 mm = 10-3 m
500 nm = 500 × 10-9 m = 5 × 10-7 m
5 × 10-7 m = (5 × 10-7 / 10-3) mm = 5 × 10-4 mm = 0.0005 mm.

LCoptical instrument ≈ 0.0005 mm

Comparing the least counts:

  • Vernier Callipers: 0.05 mm
  • Screw Gauge: 0.01 mm
  • Optical Instrument: 0.0005 mm

Since 0.0005 mm is the smallest least count, the optical instrument is the most precise device among the three.

Answer: (c) an optical instrument that can measure length to within a wavelength of light.

1.7 A student measures the thickness of a human hair by looking at it through a microscope of magnification 100. He makes 20 observations and finds that the average width of the hair in the field of view of the microscope is 3.5 mm. What is the estimate on the thickness of hair?

Given:
Magnification of the microscope M = 100.
Average observed width of the hair in the field of view = 3.5 mm.

The relationship between observed length, actual length, and magnification is:
Magnification = Observed Length / Actual Length

Rearranging to find the actual thickness of the hair:
Actual Thickness of Hair = Observed Width / Magnification
Actual Thickness = 3.5 mm / 100
Actual Thickness = 0.035 mm.

The observed width 3.5 mm has two significant figures. The magnification 100 is an exact number (or given as a whole number, implies infinite significant figures). Therefore, the result should be rounded to two significant figures.

Answer: 0.035 mm

1.8 Answer the following:
(a) You are given a thread and a metre scale. How will you estimate the diameter of the thread?
(b) A screw gauge has a pitch of 1.0 mm and 200 divisions on the circular scale. Do you think it is possible to increase the accuracy of the screw gauge arbitrarily by increasing the number of divisions on the circular scale?
(c) The mean diameter of a thin brass rod is to be measured by vernier callipers. Why is a set of 100 measurements of the diameter expected to yield a more reliable estimate than a set of 5 measurements only?

(a) How to estimate the diameter of a thread with a thread and a metre scale?

Solution: This method is known as the winding method or multiple turns method.
Wrap the thread tightly and closely around a cylindrical object (e.g., a pencil or a rod) for a large number of turns, say 20 or 50 turns, ensuring there are no gaps or overlaps between the windings. Using the metre scale, measure the total length (L) occupied by these ‘n’ turns. Since the threads are wound closely, the total length occupied by ‘n’ turns is approximately equal to ‘n’ times the diameter of a single thread.
Therefore, the diameter (d) of the thread can be estimated as:
d = Total length (L) / Number of turns (n).
This method averages out random errors and provides a more accurate estimate than trying to measure a single thread’s diameter directly with a metre scale.

(b) Is it possible to arbitrarily increase screw gauge accuracy by increasing circular divisions?

Solution: No, it is generally not possible to arbitrarily increase the accuracy of a screw gauge simply by increasing the number of divisions on its circular scale. While increasing divisions does decrease the theoretical least count (LC = Pitch / No. of divisions), practical limitations come into play. These limitations include:

  • Manufacturing Limitations: It becomes increasingly difficult and costly to manufacture scales with extremely fine, distinguishable divisions.
  • Observational Errors: The human eye has a limit to its resolution. Beyond a certain point, it becomes impossible for an observer to distinguish between very closely spaced divisions or to accurately estimate fractional parts of these divisions. This introduces human error in reading.
  • Instrumental Errors: Physical defects in the screw gauge itself, such as backlash error (play between the screw and nut) or zero error (where the zero marks don’t align perfectly), become more dominant factors affecting accuracy than the theoretical least count. These errors do not diminish with increased divisions.
  • Environmental Factors: Temperature fluctuations, vibrations, and other environmental factors can also affect the measurement precision at very high levels of supposed accuracy.

Therefore, there is a practical limit to the achievable accuracy, irrespective of the number of divisions.

(c) Why are 100 measurements more reliable than 5 for mean diameter?

Solution: Taking a larger number of measurements (e.g., 100 instead of 5) of the mean diameter of a thin brass rod with vernier callipers is expected to yield a more reliable estimate primarily due to the reduction of random errors.

  • Minimization of Random Errors: Every measurement is subject to random errors, which are unpredictable variations in readings. These can arise from slight variations in instrument positioning, fluctuating environmental conditions, or subtle inconsistencies in the observer’s reading technique. When a large number of measurements are taken, these random errors tend to cancel each other out during the averaging process. Positive errors are likely to be offset by negative errors, leading to a mean value that is closer to the true value.
  • Increased Precision: A mean calculated from a larger set of data points provides a more precise estimate of the true value. The uncertainty associated with the mean decreases as the number of observations increases (inversely proportional to the square root of the number of observations).
  • Statistical Reliability: A larger sample size provides a more robust statistical basis for the measurement. It helps in identifying and reducing the impact of any outlier readings or temporary fluctuations that might skew a smaller set of measurements.

While systematic errors (consistent errors inherent in the instrument or method) are not reduced by taking more readings, the overall reliability of the estimate is significantly enhanced by minimizing random variations.

1.9 The photograph of a house occupies an area of 1.75 cm2 on a 35 mm slide. The slide is projected on to a screen, and the area of the house on the screen is 1.55 m2. What is the linear magnification of the projector-screen arrangement.

Given:
Area of the house on the slide (object area), Aslide = 1.75 cm2.
Area of the house on the screen (image area), Ascreen = 1.55 m2.

To calculate magnification, both areas must be in the same units. Let’s convert m2 to cm2.
We know 1 m = 100 cm, so 1 m2 = (100 cm)2 = 10000 cm2 = 104 cm2.
Ascreen = 1.55 m2 = 1.55 × 104 cm2 = 15500 cm2.

The area magnification (Marea) is the ratio of the image area to the object area:
Marea = Ascreen / Aslide
Marea = 15500 cm2 / 1.75 cm2
Marea ≈ 8857.1428...

The linear magnification (Mlinear) is the square root of the area magnification:
Mlinear = √Marea
Mlinear = √8857.1428...
Mlinear ≈ 94.11239...

Both given areas (1.75 cm2 and 1.55 m2) have three significant figures. Therefore, the final answer for linear magnification should also be rounded to three significant figures.


Mlinear ≈ 94.1.

Answer: 94.1

1.10 State the number of significant figures in the following:

(a) 0.007 m2

Solution: Leading zeros (zeros before the first non-zero digit) are never significant.
The only non-zero digit is 7.

Answer: 1 significant figure

(b) 2.64 × 1024 kg

Solution: All non-zero digits are significant. The power of 10 does not affect the number of significant figures.

Answer: 3 significant figures

(c) 0.2370 g cm–3

Solution: The leading zero is not significant. All non-zero digits are significant. The trailing zero (0) after the decimal point is significant.

Answer: 4 significant figures

(d) 6.320 J

Solution: All non-zero digits are significant. The trailing zero (0) after the decimal point is significant.

Answer: 4 significant figures

(e) 6.032 N m–2

Solution: All non-zero digits are significant. The zero between non-zero digits (sandwich zero) is significant.

Answer: 4 significant figures

(f) 0.0006032 m2

Solution: The leading zeros (before 6) are not significant. The zero between non-zero digits (sandwich zero, between 6 and 3) is significant.

Answer: 4 significant figures

1.11 The length, breadth and thickness of a rectangular sheet of metal are 4.234 m, 1.005 m, and 2.01 cm respectively. Give the area and volume of the sheet to correct significant figures.

Given dimensions:
Length (L) = 4.234 m (4 significant figures)
Breadth (B) = 1.005 m (4 significant figures)
Thickness (T) = 2.01 cm (3 significant figures)

First, ensure all measurements are in the same unit. Convert thickness to meters:
T = 2.01 cm = 2.01 × 10-2 m = 0.0201 m (3 significant figures).

Calculation of Area:

The area of the rectangular sheet is given by Area = L × B.
Area = 4.234 m × 1.005 m = 4.25517 m2.

In multiplication, the result must be rounded to the least number of significant figures present in the input values. Both L and B have 4 significant figures. So, the area should be rounded to 4 significant figures.


Area ≈ 4.255 m2.

Area = 4.255 m2

Calculation of Volume:

The volume of the rectangular sheet is given by Volume = L × B × T.
Volume = 4.234 m × 1.005 m × 0.0201 m
Volume = 0.085529934 m3.

The number of significant figures in L is 4, in B is 4, and in T is 3. In multiplication, the result must be rounded to the least number of significant figures, which is 3 (from the thickness T).


Volume ≈ 0.0855 m3.

Volume = 0.0855 m3

1.12 The mass of a box measured by a grocer’s balance is 2.30 kg. Two gold pieces of masses 20.15 g and 20.17 g are added to the box. What is (a) the total mass of the box, (b) the difference in the masses of the pieces to correct significant figures?

Given masses:
Mass of box mbox = 2.30 kg (2 decimal places, 3 significant figures).
Mass of first gold piece m1 = 20.15 g (2 decimal places, 4 significant figures).
Mass of second gold piece m2 = 20.17 g (2 decimal places, 4 significant figures).

For calculations, ensure all units are consistent. Convert grams to kilograms for total mass calculation:
m1 = 20.15 g = 20.15 × 10-3 kg = 0.02015 kg.
m2 = 20.17 g = 20.17 × 10-3 kg = 0.02017 kg.

(a) Total mass of the box:

Total mass Mtotal = mbox + m1 + m2.
Mtotal = 2.30 kg + 0.02015 kg + 0.02017 kg
Mtotal = 2.34032 kg.

In addition, the result must be rounded to the least number of decimal places present in the original numbers.
mbox has 2 decimal places (2.30).
m1 and m2 (in kg) have 5 decimal places (0.02015, 0.02017).
Therefore, the total mass must be rounded to 2 decimal places.


Mtotal ≈ 2.34 kg.

Answer (a): 2.34 kg

(b) Difference in the masses of the pieces:

Difference Δm = |m2 - m1|.
Δm = |20.17 g - 20.15 g| = 0.02 g.

In subtraction, the result must be rounded to the least number of decimal places present in the original numbers. Both m1 and m2 have 2 decimal places. Therefore, the difference should also be expressed with 2 decimal places.


Δm = 0.02 g.

Answer (b): 0.02 g

1.13 A famous relation in physics relates ‘moving mass’ m to the ‘rest mass’ m0 of a particle in terms of its speed v and the speed of light, c. (This relation first arose as a consequence of special relativity due to Albert Einstein). A boy recalls the relation almost correctly but forgets where to put the constant c. He writes:
m = m0 (1 - v2)-1/2.
Guess where to put the missing c.

The principle of homogeneity of dimensions states that in a physically correct equation, the dimensions of each term on both sides of the equation must be identical. Additionally, quantities being added or subtracted must have the same dimensions, and the argument of a function (like a square root in this case) must be dimensionless.

The given equation is m = m0 (1 - v2)-1/2.

Let’s analyze the dimensions of the terms:
Dimensions of mass m and rest mass m0 are [M].

Consider the term inside the parenthesis, (1 - v2).
The number 1 is dimensionless. For subtraction to be dimensionally valid, v2 must also be dimensionless.

The dimension of speed v is [L T-1].
So, the dimension of v2 is [L2 T-2]. This is not dimensionless.

To make the term v2 dimensionless, it must be divided by another quantity that has the same dimensions as v2. The only other speed-related constant in the context of special relativity is the speed of light, c, which also has dimensions [L T-1]. Therefore, c2 has dimensions [L2 T-2].

If we divide v2 by c2, the new term (v2/c2) will be dimensionless:
Dimension of (v2/c2) = [L2 T-2] / [L2 T-2] = [M0 L0 T0] (dimensionless).

Thus, for the equation to be dimensionally consistent, the missing c must be placed as c2 in the denominator of the v2 term.

The correct relation is:
m = m0 (1 - v2/c2)-1/2
or equivalently, m = m0 / √(1 - v2/c2).

Answer: The missing ‘c’ should be ‘c2‘ in the denominator of the v2 term, making the relation m = m0 (1 - v2/c2)-1/2.

1.14 The unit of length convenient on the atomic scale is known as an angstrom and is denoted by Å: 1 Å = 10–10 m. The size of a hydrogen atom is about 0.5 Å. What is the total atomic volume in m3 of a mole of hydrogen atoms?

Given:
1 Å = 10-10 m.
Size (radius) of a hydrogen atom r = 0.5 Å.

Convert the radius to meters:
r = 0.5 × 10-10 m = 5 × 10-11 m.

Assume a hydrogen atom is spherical. The volume of a sphere is given by V = (4/3)πr3.
Volume of one hydrogen atom = (4/3) × 3.14159 × (5 × 10-11 m)3
= (4/3) × 3.14159 × (125 × 10-33 m3)
= 523.59... × 10-33 m3 ≈ 5.236 × 10-31 m3.

A mole of hydrogen atoms contains Avogadro’s number (NA) of atoms.
NA = 6.022 × 1023 atoms/mol.

Total atomic volume of a mole of hydrogen atoms = Volume of one atom × NA.
Total Volume = (5.236 × 10-31 m3) × (6.022 × 1023)
Total Volume = (5.236 × 6.022) × 10(-31 + 23) m3
Total Volume = 31.531032 × 10-8 m3
Total Volume ≈ 3.153 × 10-7 m3.

The given radius 0.5 Å has one significant figure. However, in physics problems, it’s common to assume constants like ‘size about 0.5 Å’ might imply greater precision if other values allow for it, or to give answers matching typical textbook precision (often 2 or 3 sig figs). NCERT solutions often use 3 sig figs for this answer.
Rounding to three significant figures: 3.15 × 10-7 m3.

Answer: 3.15 × 10-7 m3

1.15 One mole of an ideal gas at standard temperature and pressure occupies 22.4 L (molar volume). What is the ratio of molar volume to the atomic volume of a mole of hydrogen? (Take the size of hydrogen molecule to be about 1 Å). Why is this ratio so large?

Given:
Molar volume of ideal gas at STP, Vmolar = 22.4 L.
Convert molar volume to m3: 1 L = 10-3 m3.
Vmolar = 22.4 × 10-3 m3.

Size of hydrogen molecule = 1 Å. Since hydrogen exists as H2 molecules, its effective radius would be half of the bond length or related to the van der Waals radius. Assuming ‘size’ refers to the diameter (as is common for molecular ‘size’ when referring to packed volume), then the radius r = 0.5 Å = 0.5 × 10-10 m = 5 × 10-11 m (this implies an assumption, but consistent with 1.14).

Volume of one hydrogen molecule (assuming spherical):
Vmolecule = (4/3)πr3 = (4/3) × 3.14159 × (5 × 10-11 m)3 ≈ 5.236 × 10-31 m3.

Atomic volume of a mole of hydrogen molecules (considering molecules, not atoms, since it’s H2):
Vatomic/molecular molar = Vmolecule × NA
Vatomic/molecular molar = (5.236 × 10-31 m3) × (6.022 × 1023 mol-1)
Vatomic/molecular molar ≈ 3.153 × 10-7 m3 (This is the “atomic volume” in the context of how much actual space the atoms/molecules themselves occupy in a mole, same as Q1.14).

Ratio of molar volume to atomic volume:

Ratio = Vmolar / Vatomic/molecular molar
Ratio = (22.4 × 10-3 m3) / (3.153 × 10-7 m3)
Ratio = (22.4 / 3.153) × 10(-3 - (-7))
Ratio = 7.1043 × 104
Rounding to three significant figures (from 22.4 L and 3.153): 7.10 × 104.

Why is this ratio so large?

This ratio is exceedingly large (approximately 71,000 times) because most of the volume occupied by a gas (like an ideal gas at STP) is empty space between the molecules, not the actual volume of the molecules themselves. In a gaseous state, molecules are widely separated and move freely, occupying only a tiny fraction of the total volume. In contrast, the ‘atomic volume’ or ‘molecular molar volume’ calculated represents the actual physical space taken up by the hydrogen molecules if they were packed densely (like in a liquid or solid state). This huge difference underscores the characteristic property of gases: their low density due to the vast intermolecular distances.

Answer: Ratio ≈ 7.10 × 104. This large ratio indicates that most of the volume occupied by a gas is empty space between molecules.

1.16 Explain this common observation clearly: If you look out of the window of a fast moving train, the nearby trees, houses etc. seem to move rapidly in a direction opposite to the train’s motion, but the distant objects (hill tops, the Moon, the stars etc.) seem to be stationary. (In fact, since you are aware that you are moving, these distant objects seem to move with you).

This common observation is a phenomenon explained by relative motion and the concept of parallax or angular displacement, combined with our perception.
When you look out of a moving train, your brain interprets objects’ motion relative to your own changing position.

  • Nearby Objects: For objects that are very close to the train (like trees, houses, poles), even a small change in the train’s position results in a very large change in the angle of sight to these objects. This large angular displacement, occurring rapidly, makes them appear to rush past quickly in the opposite direction of the train’s motion. Their apparent velocity is high because their angular velocity relative to the observer is high.
  • Distant Objects: For objects that are very far away (like hilltops, the Moon, stars), a large change in the train’s position results in a very small, almost negligible, change in the angle of sight to these objects. Their angular displacement relative to the observer is extremely small, making them appear to move very slowly or seem almost stationary.

Furthermore, our brain uses cues to determine whether the observer or the observed object is moving. Since you are aware that you are the one moving with the train, your brain interprets the distant objects as moving with you, maintaining their relative positions, while the nearby objects are perceived as moving past you.

In essence, the apparent speed of an object relative to a moving observer is proportional to its angular velocity, which decreases significantly with increasing distance. Objects at “infinity” (like very distant stars) appear to have zero angular velocity relative to the observer, and thus appear stationary or to move along with the observer.

1.17 The Sun is a hot plasma (ionized matter) with its inner core at a temperature exceeding 107 K, and its outer surface at a temperature of about 6000 K. At these high temperatures, no substance remains in a solid or liquid phase. In what range do you expect the mass density of the Sun to be, in the range of densities of solids and liquids or gases? Check if your guess is correct from the following data: mass of the Sun = 2.0 × 1030 kg, radius of the Sun = 7.0 × 108 m.

Initial Guess about Density:

Given the extremely high temperatures (millions of Kelvin in the core and thousands on the surface), one might intuitively expect the Sun’s density to be in the range of gases, as all matter would be in a gaseous or plasma state. Densities of gases at standard conditions are typically around 0.1 to 10 kg/m3.

However, the Sun is an enormous celestial body held together by immense gravitational forces. These forces cause extreme compression, especially towards the core. This compression tends to pack the matter (even plasma) very densely, counteracting the expansion due to high temperature.

Therefore, it is reasonable to expect the mass density of the Sun to be in the range of densities of **solids and liquids**, which are typically 103 to 104 kg/m3 or more.

Calculation to Check the Guess:

Given data:
Mass of the Sun M = 2.0 × 1030 kg (2 significant figures).
Radius of the Sun R = 7.0 × 108 m (2 significant figures).

The volume of the Sun (assuming it is a sphere) is V = (4/3)πR3.
V = (4/3) × 3.14159 × (7.0 × 108 m)3
V = (4/3) × 3.14159 × (7.0)3 × (108)3 m3
V = (4/3) × 3.14159 × 343 × 1024 m3
V = 1436.755 × 1024 m3 ≈ 1.437 × 1027 m3 (retaining more precision for intermediate step).

Now, calculate the average mass density (ρ = M/V):
ρ = (2.0 × 1030 kg) / (1.437 × 1027 m3)
ρ = (2.0 / 1.437) × 10(30 - 27) kg m-3
ρ = 1.3917... × 103 kg m-3.

Since both the mass and radius are given with two significant figures, the final density should be rounded to two significant figures.


ρ ≈ 1.4 × 103 kg m-3.

Conclusion:

The calculated average density of the Sun is approximately 1.4 × 103 kg m-3 or 1400 kg/m3.
This value falls well within the typical range of densities for solids and liquids (e.g., water density is 1000 kg/m3, common metals are several thousand kg/m3), and is vastly higher than the densities of gases (typically around 1 kg/m3 at standard conditions).
Therefore, the guess is correct. The immense gravitational compression in the Sun overrides the expansion due to high temperature, resulting in a very high density.

Answer: The mass density of the Sun is in the range of densities of solids and liquids, approximately 1.4 × 103 kg m-3.