Topics
Units and Measurements
- Quantitative Science
- System of Units
- Derived Quantities and Units
- Rules and Conventions for Writing SI Units and Their Symbols
- Measurement of Length
- Measurement of Mass
- Measurement of Time
- Dimensions and Dimensional Analysis
- Accuracy, Precision and Uncertainty in Measurement
- Errors in Measurements>Systematic Errors
- Errors in Measurements>Random Errors
- Estimation of Errors
- Combination of Errors
- Significant Figures
- Definitions of SI Units and Constants
Mathematical Methods
- Vector Analysis
- Scalar
- Vector
- Vector Operations>Multiplication of a Vector by a Scalar
- Vector Operations>Addition and Subtraction of Vectors
- Vector Operations>Triangle Law for Vector Addition
- Vector Operations>Law of parallelogram of vectors
- Resolution of Vectors
- Multiplication of Vectors
- Scalar Product(Dot Product)
- Vector Product (Cross Product)
- Concept of Calculus
- Differential Calculus
- Integral Calculus
Motion in a Plane
- Concept of Motion
- Rectilinear Motion
- Displacement
- Path Length
- Average Velocity
- Average Speed
- Instantaneous Velocity
- Instantaneous Speed
- Acceleration in Linear Motion
- Relative Velocity
- Motion in Two Dimensions-Motion in a Plane
- Average and Instantaneous Velocities
- Acceleration in a Plane
- Equations of Motion in a Plane with Constant Acceleration
- Relative Velocity in Two Dimensions
- Projectile Motion
- Uniform Circular Motion (UCM)
- Key Parameters of Circular Motion
- Centripetal Acceleration
- Conical Pendulum
Laws of Motion
- Fundamental Principles of Motion and Mechanics
- Types of Motion
- Aristotle’s Fallacy
- Newton’s Laws of Motion
- Newton's First Law of Motion
- Newton’s Second Law of Motion
- Newton's Third Law of Motion
- Inertial and Non-inertial Frames of Reference
- Types of Forces>Fundamental Forces in Nature
- Types of Forces>Contact and Non-Contact Forces
- Types of Forces>Real and Pseudo Forces
- Types of Forces>Conservative and Non-Conservative Forces
- Types of Forces>Work Done by a Variable Force
- Work Energy Theorem
- Principle of Conservation of Linear Momentum
- Collisions
- Elastic and Inelastic Collisions
- Perfectly Inelastic Collision
- Coefficient of Restitution e
- Expressions for Final Velocities in Elastic Head-On Collision
- Loss of Kinetic Energy in Perfectly Inelastic Head-On Collision
- Collision in Two Dimensions
- Impulse of a Force
- Necessity of Defining Impulse
- Rotational Analogue of a Force: Moment of a Force Or Torque
- Couple and Its Torque
- Proof of Independence of the Axis of Rotation
- Mechanical Equilibrium
- States of Equilibrium
- Centre of Mass>Mathematical Understanding of Centre of Mass
- Centre of Mass>Velocity of Centre of Mass
- Centre of Mass>Acceleration of Centre of Mass
- Centre of Mass>Characteristics of Centre of Mass
- Centre of Gravity
Gravitation
- Concept of Gravitation
- Kepler’s Laws
- Law of Orbit or Kepler's First Law
- Law of Areas or Kepler's Second Law
- Law of Periods or Kepler's Third Law
- Newton's Universal Law of Gravitation
- Measurement of the Gravitational Constant (G)
- Acceleration Due to Gravity (Earth’s Gravitational Acceleration)
- Variation in the Acceleration>Variation in Gravity with Altitude
- Variation in the Acceleration>Variation in Gravity with Depth
- Variation in the Acceleration>Variation in Gravity with Latitude and Rotation of the Earth
- Variation in the Acceleration>Effect of the shape of the Earth
- Gravitational Potential Energy
- Expression for Gravitational Potential Energy
- Connection of Potential Energy Formula with mgh
- Potential and Potential Difference
- Escape Velocity
- Earth Satellites
- Projection of Satellite
- Weightlessness in a Satellite
- Time Period of Satellite
- Binding Energy of an Orbiting Satellite
Mechanical Properties of Solids
- Mechanical Properties of Solids
- Elastic Behavior of Solids
- Stress and Strain
- Types of Stress and Corresponding Strain
- Hooke’s Law
- Elastic Modulus>Young’s Modulus
- Elastic Modulus>Bulk Modulus
- Elastic Modulus>Modulus of Rigidity
- Elastic Modulus>Poisson’s Ratio
- Stress-strain Curve
- Strain Energy
- Hardness of Material
- Friction in Solids
- Origin of Friction
- Types of Friction>Static Friction
- Types of Friction>Kinetic Friction
- Types of Friction>Rolling Friction
Thermal Properties of Matter
- Thermal Properties of Matter
- Temperature and Heat
- Measurement of Temperature
- Absolute Zero and Absolute Temperature
- Ideal Gas Equation
- Thermal Expansion
- Linear Expansion
- Areal Expansion
- Volume Expansion
- Relation Between Coefficient of Expansion
- Specific Heat Capacity
- Specific Heat Capacity of Solids and Liquids
- Specific Heat Capacity of Gas
- Heat Equation
- Thermal Capacity
- Calorimetry
- Change of State
- Analysis of Observation>From Point A to B
- Analysis of Observation>From Point B to D
- Temperature Effects and Considerations
- Evaporation vs Boiling
- Boiling Point and Pressure
- Factors Affecting Cooking
- Sublimation
- Phase Diagram
- Gas and Vapour
- Latent Heat
- Heat Transfer
- Conduction
- Thermal Conductivity
- Coefficient of Thermal Conductivity
- Thermal Resistance
- Applications of Thermal conductivity
- Convection
- Application of Convection
- Free and Forced Convection
- Radiation
- Newton’s Law of Cooling
Sound
- Sound Waves
- Common Properties of All Waves
- Transverse Waves
- Longitudinal Waves
- Mathematical Expression of a Wave
- The Speed of Travelling Waves
- The Speed of Transverse Waves
- The Speed of Longitudinal Waves
- Newton's Formula for Velocity of Sound
- Laplace’s Correction
- Factors Affecting Speed of Sound
- Principle of Superposition of Waves
- Echo
- Reverberation
- Acoustics
- Qualities of Sound
- Doppler Effect
- Source Moving and Listener Stationary
- Listener Approaching a Stationary Source with Velocity
- Both Source and Listener are Moving
- Common Properties between Doppler Effect of Sound and Light
- Major Differences between Doppler Effects of Sound and Light
Optics
- Fundamental Concepts of Light
- Nature of Light
- Ray Optics Or Geometrical Optics
- Cartesian Sign Convention
- Reflection>Reflection from a Plane Surface
- Reflection>Reflection from Curved Mirrors
- Total Internal Reflection
- Refraction of Light
- Applications of Total Internal Reflection
- Refraction at a Spherical Surface and Lenses
- Thin Lenses and Their Combination
- Refraction at a Single Spherical Surface
- Lens Makers' Equation
- Dispersion of Light
- Analysis of Prism
- Thin Prisms
- Some Natural Phenomena Due to Sunlight
- Defects of Lenses
- Optical Instruments
- Simple Microscope or a Reading Glass
- Compound Microscope
- Telescope
Electrostatics
- Concept of Electrostatics
- Electric Charge
- Basic Properties of Electric Charge
- Additive Nature of Charge
- Quantization of Charge
- Conservation of Charge
- Force between Charges
- Coulomb’s Law
- Scalar Form of Coulomb’s Law
- Relative Permittivity or Dielectric Constant
- Definition of Unit Charge from the Coulomb’s Law
- Coulomb's Law in Vector Form
- Principle of Superposition
- Electric Field
- Electric Field Intensity Due to a Point-Charge
- Practical Way of Calculating Electric Field
- Electric Lines of Force
- Electric Flux
- Gauss’s Law
- Electric Dipole
- Couple Acting on an Electric Dipole in a Uniform Electric Field
- Electric Intensity at a Point Due to an Electric Dipole
- Continuous Charge Distribution
Electric Current Through Conductors
- Concept of Electric Currents in Conductors
- Electric Current
- Flow of Current Through a Conductor
- Drift Speed
- Ohm's Law
- Limitations of Ohm’s Law
- Electrical Power
- Resistors
- Rheostat
- A combination of resistors in both series and parallel
- Specific Resistance
- Variation of Resistance with Temperature
- Electromotive Force (emf)
- Cells in Series
- Cells in Parallel
- Types of Cells
Magnetism
- Concept of Magnetism
- Magnetic Lines of Force
- The Bar Magnet
- Magnetic Field due to a Bar Magnet
- Magnetic Field Due to a Bar Magnet at an Arbitrary Point
- Gauss' Law of Magnetism
- The Earth’s Magnetism
Electromagnetic Waves and Communication System
- Foundations of Electromagnetic Theory
- EM Wave
- Sources of EM Waves
- Characteristics of EM Waves
- Electromagnetic Spectrum
- Radio Waves
- Microwaves
- Infrared waves
- Visible Light
- Ultraviolet rays
- X-rays
- Gamma Rays
- Propagation of EM Waves
- Ground (surface) Wave
- Space wave
- Sky wave propagation
- Communication System
- Elements of a Communication System
- Commonly Used Terms in Electronic Communication System
- Modulation
Semiconductors
- Concept of Semiconductors
- Electrical Conduction in Solids
- Band Theory of Solids
- Intrinsic Semiconductor
- Extrinsic Semiconductor
- n-type semiconductor
- p-type semiconductor
- Charge neutrality of extrinsic semiconductors
- p-n Junction
- A p-n Junction Diode
- Basics of Semiconductor Devices
- Applications of Semiconductors and P-n Junction Diode
- Thermistor
- Introduction
- Formula: Pseudo-Forces
- Characteristics
- Understanding Pseudo Forces
- Significance
- Example
- Real-Life Examples
Introduction
In physics, forces are not always what they seem when we observe them from moving reference frames. When you ride in an accelerating lift or bus, you feel pushed down or sideways, but these feelings have a special explanation. These mysterious forces appear and disappear depending on whether you're observing from a stationary ground or from inside a moving vehicle. Understanding real and pseudo forces helps us apply Newton's laws correctly in any situation, whether we are at rest or moving with acceleration. This concept is crucial for solving real-world problems involving motion in accelerating systems.
Formula: Pseudo Forces
Pseudo Force: Fpseudo = −m\[\vec a\]
Where:
- m = mass of the object
- \[\vec a\] = acceleration of the non-inertial reference frame
- The negative sign indicates the force is opposite to the acceleration direction
Characteristics
- Measurable: Pseudo-forces can be detected using instruments like weighing scales
- Non-fundamental: They are not among the four fundamental forces
- Frame-dependent: They exist only in non-inertial (accelerated) reference frames
- Direction: Always opposite to the acceleration of the reference frame
- Magnitude: Equal to −m\[\vec a\]
- Not imaginary: They produce real, measurable effects on objects and measuring devices
- Enable Newton's Laws: Adding pseudo forces allows us to apply Newton's laws in accelerated frames
Understanding Pseudo Forces
The concept works as follows:
- You observe motion from inside an accelerating vehicle (non-inertial frame)
- Objects appear to experience forces that don't exist in a stationary observer's view
- These apparent forces are pseudo-forces
- Adding the term −m\[\vec a\] to Newton's second law allows us to use it in accelerated frames
- Pseudo forces always point opposite to the acceleration direction
Significance
- Practical Problem-Solving: Allows us to analyze motion from any reference frame, including accelerated ones
- Safety Applications: Helps engineers design elevators, vehicles, and roller coasters, considering apparent forces
- Understanding Motion: Explains why we feel different sensations during acceleration in vehicles or elevators
- Mathematical Tool: Enables the use of Newton's laws in non-inertial frames without complex calculations
- Real-World Design: Essential for designing safety systems, G-force measurements, and acceleration-based devices
- Conceptual Clarity: Distinguishes between real fundamental forces and apparent forces in accelerated systems
Example
A car of mass 1.5 tons is running at 72 kmph on a straight horizontal road. On turning the engine off, it stops in 20 seconds. While running at the same speed, on the same road, the driver observes an accident 50 m in front of him. He immediately applies the brakes and just manages to stop the car at the accident spot. Calculate the braking force.
Step-by-Step Solution:
Find the frictional retardation (when the engine turns off)
- Initial velocity: u = 72 kmph = 20 m/s
- Final velocity: v = 0
- Time: t = 20 s
- Using a = \[\frac {v−u}{t}\]:
a = \[\frac {0−20}{20}\] = −1 m/s2 - This is frictional retardation (negative acceleration)
Find total retardation (when brakes are applied)
- Initial velocity: u = 20 m/s
- Final velocity: v = 0
- Distance: s = 50 m
- Using a1 = \[\frac {v^2 − u^2}{2s}\]:
a1 = \[\frac {0 − 400}{2 × 50}\] = \[\frac {−400}{100}\] = −4 m/s2
Calculate braking retardation alone
- Total retardation = Braking retardation + Frictional retardation
- Braking retardation = 4 - 1 = 3 m/s²
Calculate braking force
- Convert mass: 1.5 ton = 1500 kg
- Using Force = mass × acceleration:
Braking force = 1500 × 3 = 4500 N
Real-Life Examples
1. Elevator Scenarios
- When an elevator suddenly moves up, people feel heavier (apparent weight increases)
- When an elevator descends with deceleration, people feel lighter
- Astronauts in a spacecraft experience weightlessness because the spacecraft accelerates downward at gg, making the pseudo force cancel gravity
2. Vehicle Safety
- Car airbags deploy during sudden braking because passengers experience a pseudo force pushing them forward
- Seat belts are designed to counteract the pseudo force during acceleration or deceleration
- Anti-lock braking systems (ABS) work by managing the pseudo forces during braking
3. Roller Coaster Thrills
- During loops, riders feel heavier at the bottom (upward acceleration) and lighter at the top (downward acceleration)
- The sensation of being pushed against seats or feeling weightless is due to pseudo-forces
4. Aircraft Motion
- During takeoff, passengers feel pushed back into their seats (pseudo force)
- During landing and deceleration, passengers lean forward due to the pseudo force
- Fighter pilots experience extreme g-forces (pseudo-forces) during maneuvers
5. Planetary Motion
-
Objects on Earth's rotating surface experience centrifugal pseudo force, which is why we weigh slightly less at the equator than at the poles
