Q1. Study the entries in the table and rewrite them by placing matching items in one row
Answer: (Table content would be displayed here based on textbook)
Note:
The PDF image didn't export the table contents clearly. If you provide the table data as text or an image, I'll format it properly in the table below.
| Concept | Definition/Formula | Example/Application |
|---|---|---|
| Mass | Amount of matter in a body (kg) | 5 kg object |
| Weight | Force due to gravity (N) | 49 N on Earth |
| Free Fall | Motion under gravity alone | Dropped stone |
| g (gravity) | 9.8 m/s² on Earth | Acceleration of falling objects |
Q2. Answer the following questions
A. What is the difference between the mass and weight of an object? Will their values remain the same on Mars as on Earth? Explain.
Answer:
Here are the key differences between mass and weight:
| Mass | Weight |
|---|---|
| Amount of matter in a body (like blood, bones, tissues, etc.) | Force exerted on a body due to gravity |
| Scalar quantity (magnitude only) | Vector quantity (has magnitude and direction toward center of planet) |
| SI unit: kilogram (kg) | SI unit: newton (N) |
| Measured using balance | Measured using spring balance |
| Constant everywhere | Varies with location and gravitational acceleration |
On Mars vs Earth:
- Mass: Since the amount of matter does not change with location, the mass of any object remains the same on both Earth and Mars.
- Weight: However, weight depends on the gravitational pull acting on the body. Because the gravitational acceleration (g) is not the same on Earth and Mars, the weight of the object differs on the two planets.
- Formula: Weight = Mass × g
- On Mars, g ≈ 3.7 m/s² (about 38% of Earth's g = 9.8 m/s²), so weight on Mars would be approximately 38% of weight on Earth.
B. What are (i) free fall, (ii) acceleration due to gravity, (iii) escape velocity, and (iv) centripetal force?
Answer:
(i) Free Fall:
A body is said to be in free fall when it moves only under gravity's influence, with no other external force acting on it (except gravity). In such motion:
- The object starts with zero initial velocity (if simply dropped)
- Air resistance affects it in reality, so perfect free fall is possible only in a vacuum
- All objects in free fall accelerate at the same rate regardless of their mass (Galileo's principle)
Examples:
- A stone dropped from a table falls due to gravity alone
- A fruit dropping from a tree
- Astronauts in orbit experience "weightlessness" which is continuous free fall around Earth
Not free fall: Standing on the ground or sitting in an aircraft is not free fall because several forces act besides gravity.
(ii) Acceleration due to gravity (g):
This is the acceleration produced in an object due to the Earth's gravitational pull.
- SI unit: m/s²
- Represented by symbol: g
- Value on Earth's surface: approximately 9.8 m/s² (varies slightly with altitude and latitude)
- It is a vector quantity directed toward the Earth's centre
- On the Moon: 1.63 m/s² (about one-sixth of Earth's value)
- On Mars: 3.7 m/s²
- Formula: g = GM/R² where G is gravitational constant, M is Earth's mass, R is Earth's radius
(iii) Escape Velocity:
Escape velocity is the minimum initial speed required by an object to break free from a planet's gravitational force and never return (reach infinite distance with zero final velocity).
- On Earth: 11.186 km/s (approximately 11.2 km/s)
- Formula: vₑ = √(2GM/R)
- On Moon: 2.38 km/s (much lower due to smaller mass)
- Satellites and rockets are launched with speeds equal to or greater than escape velocity so they can leave Earth's gravitational influence
- Escape velocity depends on the mass and radius of the celestial body but is independent of the mass of the escaping object
(iv) Centripetal Force:
This is the force that pulls an object toward the centre of the circular path in which it moves, keeping it in circular motion.
- It is directed inward toward the rotation centre
- Formula: F = mv²/r or F = mω²r
- In planetary motion, gravitational force provides the centripetal force that keeps planets in orbit
Example: A stone tied to a string moves in a circle because the tension in the string provides the centripetal force. If the string breaks, the stone flies off tangentially (Newton's First Law).
C. State Kepler's three laws. How did these laws help Newton to derive the inverse-square law of gravity?
Answer:
Johannes Kepler (1571-1630) analyzed the precise astronomical observations of Tycho Brahe and found that planetary movements follow certain mathematical rules. Based on these observations, he proposed three fundamental laws known as Kepler's Laws of Planetary Motion:
Kepler's First Law (Law of Ellipses):
A planet revolves around the Sun in an elliptical path, and the Sun occupies one of its foci.
- This rejected the ancient belief of circular orbits
- The ellipse has two foci, and the Sun is at one focus (not the center)
- The degree of elongation is measured by eccentricity (e)
Kepler's Second Law (Law of Equal Areas):
The line joining a planet and the Sun (radius vector) sweeps out equal areas in equal time intervals.
- This means planets move faster when closer to the Sun (perihelion) and slower when farther (aphelion)
- This is a consequence of conservation of angular momentum
- Area swept per unit time = constant
Kepler's Third Law (Harmonic Law):
The square of a planet's orbital period (T²) is directly proportional to the cube of the semi-major axis of its orbit (a³).
T² ∝ a³ or T²/a³ = constant for all planets orbiting the same star
- This law relates orbital period to distance from Sun
- The constant is the same for all planets orbiting the Sun
- Example: A planet 4 times farther from Sun takes 8 times longer to orbit (4³ = 64, √64 = 8)
How these helped Newton:
Sir Isaac Newton (1643-1727) used Kepler's laws as crucial evidence for his Universal Law of Gravitation:
- From Kepler's third law (T² ∝ r³) and assuming circular orbits for simplicity
- Using centripetal force formula: F = mv²/r
- Orbital velocity: v = 2πr/T
- Combining these: F ∝ m/r² (for same central body)
- By symmetry and Newton's Third Law: F ∝ M/r² (for same orbiting body)
- Thus: F ∝ Mm/r² or F = G Mm/r²
Newton thus mathematically showed that the gravitational force between two bodies decreases with the square of the distance between them (inverse-square law). He also proposed that this is a universal law applying to all masses in the universe.
D. A stone is thrown straight upward with initial velocity u and reaches height h before falling. Show that the time for upward motion equals the time for downward motion.
Proof:
Let the stone move upward with initial velocity u and rise to maximum height h.
Time taken to rise (t₁):
Using the first equation of motion:
At the topmost point (maximum height):
- Final velocity v = 0
- Acceleration a = -g (gravity acts downward, opposite to upward motion)
Time taken to fall (t₂):
For downward motion from height h:
- Initial velocity = 0 (starts from rest at top)
- Acceleration = +g (downward direction, same as motion)
- Distance = h
Using second equation of motion:
Relation between u and h:
Using third equation of motion for upward path:
Substitute u into t₁:
Compare t₁ and t₂:
Thus, the ascent time equals the descent time: t₁ = t₂
This result assumes no air resistance and constant g. In reality, air resistance makes descent slightly longer due to reduced net acceleration.
E. If g suddenly becomes twice its original value, pulling a heavy object becomes twice as difficult. Why?
Answer:
The force needed to lift or pull an object horizontally against friction depends on its weight:
Original situation:
Weight of object: W₁ = mg
Force of friction (which opposes motion): F_friction = μN = μmg
Where:
- μ = coefficient of friction
- N = mg = normal force (equal to weight for horizontal surface)
Force needed to pull: F₁ = μmg (to overcome friction)
When g doubles:
New weight: W₂ = m(2g) = 2mg
New frictional force: F_friction_new = μ(2mg) = 2μmg
Force needed to pull: F₂ = 2μmg = 2F₁
Thus, when g becomes two times greater, the required pulling force also becomes double, making it twice as difficult to pull a heavy body across the floor.
Additional insight: This applies to:
- Lifting objects vertically: Force needed = weight = mg, so doubles when g doubles
- Pulling horizontally: Force needed to overcome friction ∝ normal force ∝ weight ∝ g
- Even the effort to hold an object stationary increases proportionally with g
Q3. Explain why g becomes zero at the Earth's centre
Explanation:
The value of gravitational acceleration g depends on:
- The Earth's mass (M) that effectively attracts the object
- The distance (R) from the Earth's centre to the object
Formula: g = GM/R² (outside or on surface)
As we move toward the Earth's centre:
1. Effective Mass Decreases:
Only the mass inside the spherical shell at your current radius contributes to gravity. The mass in outer shells exerts no net gravitational force on an object inside them (shell theorem proved by Newton).
2. Distance Decreases:
As R decreases, the 1/R² factor would normally increase g, but the decreasing effective mass counteracts this.
Mathematical Derivation:
For uniform density Earth (approximation):
Thus inside Earth: g ∝ R
At different positions:
- At surface (R = R_earth): g = 9.8 m/s²
- At half radius (R = R_earth/2): g ≈ 4.9 m/s²
- At quarter radius (R = R_earth/4): g ≈ 2.45 m/s²
- As R → 0: g → 0
At the exact centre (R = 0):
- All Earth's mass is symmetrically distributed around you
- Gravitational pulls from all directions cancel each other completely
- Net gravitational force = 0
- Thus g = 0 at Earth's centre
Real Earth consideration: Earth's density increases toward the core, so g initially increases slightly before decreasing to zero, but still reaches zero at centre.
Q4. If a planet's orbital period at distance R from a star is T, prove that at distance 2R, its period becomes √8 T
Proof:
According to Kepler's third law of planetary motion:
or
where k is a constant for planets orbiting the same star.
Given:
- Initial distance: r₁ = R
- Initial period: T₁ = T
- New distance: r₂ = 2R
- New period: T₂ = ?
Applying Kepler's third law:
Cross-multiplying:
Taking square root:
Thus, at twice the distance, the orbital period becomes √8 times (approximately 2.83 times) the original period.
Verification: This makes sense intuitively - farther planets move slower and take much longer to complete orbits. For example, Mars (1.5 AU from Sun) takes 1.88 Earth years, while Earth (1 AU) takes 1 year.
Q5. Solve the following examples
A. An object falls from a height of 5 m on a planet and takes 5 s to reach the ground. Find g for that planet.
Solution:
Given:
- Height: s = 5 m
- Time: t = 5 s
- Initial velocity: u = 0 (dropped from rest)
Using second equation of motion:
Thus, gravitational acceleration on that planet is 0.4 m/s², which is about 1/24th of Earth's g.
B. Planet A has radius half that of planet B. If A has mass Mₐ, what must be mass of B so that g on B is half of that on A?
Solution:
Gravitational acceleration formula:
For planet A:
For planet B:
Given:
- Rₐ = ½ R_b or R_b = 2Rₐ
- g_b = ½ gₐ
Substitute into g_b formula:
But gₐ = GMₐ/Rₐ², so substitute:
Cancel common terms (G and Rₐ²):
Solve for M_b:
Thus, planet B must have twice the mass of planet A to have half the surface gravity, given that its radius is double.
C. An object has mass 5 kg and weight 49 N on Earth. What are its values on the Moon (g = 1/6 that of Earth)?
Solution:
Mass:
Mass remains unchanged everywhere as it is the amount of matter.
Weight on Earth:
Given: Weight on Earth = 49 N
Weight on Moon:
Given: g_moon = (1/6) g_earth = (1/6) × 9.8 ≈ 1.633 m/s²
Answer:
- Mass on Moon: 5 kg (same as on Earth)
- Weight on Moon: 8.17 N (about 1/6 of Earth weight)
D. A body thrown upward reaches 500 m. Find initial speed and time to return. Take g = 10 m/s².
Solution:
Given:
- Maximum height: h = 500 m
- Gravity: g = 10 m/s²
- At maximum height: v = 0
1. Find initial speed (u):
Using third equation of motion:
2. Find ascent time (t_up):
Using first equation of motion:
3. Total time of flight:
From symmetry (proved in Q2D), time of ascent = time of descent
Answer:
- Initial speed: 100 m/s
- Total time to return: 20 seconds
E. A ball falls from a table and hits the ground in 1 s. If g = 10 m/s², find its speed on reaching the ground and the height of the table.
Solution:
Given:
- Time of fall: t = 1 s
- Gravity: g = 10 m/s²
- Initial velocity: u = 0 (dropped, not thrown)
1. Final speed on reaching ground:
Using first equation of motion:
2. Height of table:
Using second equation of motion:
Answer:
- Speed on impact: 10 m/s
- Height of table: 5 meters
F. Calculate the gravitational force between Earth and Moon.
Mass of Earth = 6 × 10²⁴ kg
Mass of Moon = 7.4 × 10²² kg
Distance = 3.84 × 10⁵ km
G = 6.7 × 10⁻¹¹ N m²/kg²
Solution:
Step 1: Convert distance to meters
Step 2: Apply Newton's Law of Universal Gravitation
Step 3: Substitute values
Step 4: Calculate numerator
Step 5: Calculate denominator
Step 6: Final calculation
Answer: The gravitational force between Earth and Moon is approximately 2.02 × 10²⁰ N.
This enormous force (about 20 followed by 19 zeros newtons) is what keeps the Moon in orbit around Earth.
G. Mass of Earth = 6 × 10²⁴ kg
Distance to Sun = 1.5 × 10¹¹ m
Gravitational force = 3.5 × 10²² N
Find Sun's mass.
G = 6.7 × 10⁻¹¹ N m²/kg²
Solution:
Step 1: Write Newton's Law of Universal Gravitation
Step 2: Rearrange for Sun's mass (M_sun)
Step 3: Substitute given values
Step 4: Calculate numerator
Step 5: Calculate denominator
Step 6: Final calculation
Answer: The mass of the Sun is approximately 1.96 × 10³⁰ kg.
This is about 330,000 times the mass of Earth, which matches known astronomical values.