Force, Newton’s laws of Motion, gravitation
Force and Motion
Introduction to Force
- In the previous chapter, motion was studied.
- This chapter focuses on the cause of motion: force.
- Philosophers believed continuous force was needed for continuous motion.
- It was known that force could initiate or halt motion.
- The precise meaning of force was unclear to scholars of the past.
- They formulated theories but didn't verify them through experimentation.
Galileo's Experimental Approach
- Galileo Galilei pioneered the study of motion using experiments.
- He used simple tools like clocks to study motion with precision.
- Mathematics was not well-developed, and equations were not commonly used at the time.
- Galileo formulated rules using ratios and proportions.
- For uniform motion, he stated, 'distance covered and time taken are directly proportional.'
- Galileo's work significantly improved the understanding of motion concepts.
- He studied linear, oscillatory, and projectile motion.
Sir Isaac Newton's Contributions
- Sir Isaac Newton (1642-1727) was an influential physicist, mathematician, astronomer, philosopher, alchemist, and theologian.
- He is considered one of history's greatest and most influential scientists.
- His book ‘Philosophiæ Naturalis Principia Mathematica’ (1687) laid the groundwork for classical mechanics.
- Newton described universal gravitation and the three laws of motion.
Newton’s Laws of Motion
- Newton's laws relate forces acting on a body to its motion.
- These laws can be summarized into three statements.
First Law: The Law of Inertia
- A body's velocity remains constant unless acted upon by an external force.
- Inertia is the property of bodies to resist changes in their state of motion.
- A body at rest stays at rest, and a body in uniform motion stays in uniform motion unless a force acts upon it.
- Example: A marble rolling on a frictionless surface would continue to roll forever.
- In reality, friction between the marble and the surface causes it to stop.
- Inertia is directly proportional to mass: more mass implies more inertia.
- Examples of inertia in daily life:
- A book on a table stays there unless an external force moves it.
- Passengers in a starting bus feel thrown backward due to inertia of rest.
- Passengers in a stopping bus are thrown forward due to inertia of motion.
- Dust is removed from a carpet beaten with a stick because dust particles resist the change in motion.
- A cyclist continues moving for a while after pedaling stops.
- A person jumping from a moving vehicle must run to avoid falling.
Second Law: Rate of Change of Momentum
- The rate of change of momentum is proportional to the external unbalanced force, and the change occurs in the force's direction.
- The mass is assumed constant during the force application.
- Formula: Force = \frac{change \ in \ momentum}{time}
- F = \frac{mv - mu}{t}, where:
- m = mass,
- v = final velocity,
- u = initial velocity,
- t = time.
- F = m \frac{(v-u)}{t}
- F = ma, since \frac{(v-u)}{t} = a (acceleration).
- The unit of force is the Newton (N).
- 1 Newton is the force that produces an acceleration of 1 m/s^2 when applied to a mass of 1 kg.
- The unit of force in the CGS system is the dyne.
- 1 dyne is the force that produces an acceleration of 1 cm/s^2 when applied to a mass of 1 g.
Third Law: Action and Reaction
- For every action (force), there is an equal and opposite reaction (force).
- Action and reaction forces act on different bodies.
- Examples:
- A rocket expels hot gases backward (action), and the gases push the rocket forward (reaction).
- A swimmer pushes water back (action), and water pushes the swimmer forward.
- While walking, we push the ground back (action), and the ground pushes us forward.
- When a bullet is fired from a gun, the gun recoils backward.
Newton’s Law of Gravitation
- Every point mass attracts every other point mass in the universe.
- The force is directly proportional to the product of their masses and inversely proportional to the square of the distance between them.
- Formula: F \propto \frac{m1 m2}{r^2}
- F = G \frac{m1 m2}{r^2}, where:
- m1 and m2 are the masses,
- r is the distance between the masses,
- G is the universal gravitational constant.
- The value of G was measured by Henry Cavendish in 1798: G = 6.67 \times 10^{-11} Nm^2/kg^2.
Gravitational Acceleration
- When an object is dropped, Earth applies gravitational force, accelerating it toward the ground.
- This acceleration is called gravitational acceleration ('g').
- The value of 'g' depends on the distance from the Earth's center.
- By Newton's second law: F = ma
- Gravitational force = mass x gravitational acceleration.
- G \frac{m1 mE}{r^2} = m \times g, where:
- m_E is the mass of the Earth,
- r is the distance between the object and the Earth's center.
- g = G \frac{m_E}{r^2}
- Substituting m_E = 5.98 \times 10^{24} kg and r = 6.37 \times 10^6 m, we get g = 9.8 m/s^2 on Earth.
- 'g' depends on the mass and radius of the Earth but not on the object's mass.
- All objects experience the same gravitational acceleration.
- A larger and smaller stone dropped from the same height will reach the ground at the same time.
- The Earth's radius is greater at the equator than at the poles, so 'g' varies:
- g(equator) = 9.780 m/s^2
- g(pole) = 9.832 m/s^2
Mass vs. Weight
- Mass is the quantity of matter in an object.
- All objects have mass, measurable in kg.
- Weight is the gravitational force exerted on an object by Earth.
- Weight is a force and is measured in Newtons.
- Weight depends on the object's distance from the Earth's center and can vary.
- Mass remains constant regardless of location.
- Weight = gravitational force between object and Earth.
- W = G \frac{m1 mE}{r^2}, But we know that g = G \frac{m_E}{r^2}
- Hence w = mg, where g = 9.8 m/s^2.
- Weight (in Newtons) = mass (in kg) x 9.8.
- The weight of a 1 kg mass is 9.8 N.
- Saying