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WORK, ENERGY, POWER AND COLLISION
▢ Work:
❖ Definition: Work is done when a body undergoes displacement under action of force
❖ Zero Work Examples:
- •Man pushes object but displacement = 0
- •Man rows boat upstream but remains at rest w.r.t. shore
- •Centripetal force in circular motion
- •Gravitational pull on satellite in circular orbit
- •Person carrying load on head on horizontal road
- •Car moving with uniform speed on frictionless road
❖ Formulae:
Table 1: Work Done
Case | Formula |
|---|---|
Constant force | |
Variable force | |
Work-energy theorem | |
SI unit | Joule |
CGS unit | Erg |
Conversion |
❖ Sign of Work:
Table 1: Positive, Negative and Zero Work
Work | Example | |
|---|---|---|
Positive | Force supports displacement | |
Negative | Friction; gravity during upward motion | |
Zero | Centripetal force |
❖ Important Points:
- •Work is scalar
- •Work done does not depend on time taken
- •Work done by a body → energy decreases
- •Work done on a body → energy increases
▢ Power:
❖ Definition: Rate of doing work
Table 1: Power Formulae
Quantity | Formula / Unit |
|---|---|
Power | |
Using force and displacement | |
Instantaneous power | |
Rate of energy change | |
SI unit | Watt |
1 Watt | |
Practical unit | Horse power / HP |
1 HP |
▢ Energy:
❖ Definition: Capacity of a body to do work
❖ Nature:
- •Scalar quantity
- •Same units and dimensions as work
- •Mechanical energy = kinetic energy + potential energy
❖ Kinetic Energy:
◉ Definition: Energy possessed by body due to motion
Table 1: Kinetic Energy Formulae
Quantity | Formula / Point |
|---|---|
Kinetic energy | |
In terms of momentum | |
Momentum | |
Frame dependence | K.E. depends on frame of reference |
◉ Frame Example:
◉ Stopping by Same Force:
Table 1: Stopping Distance and Time
Quantity | Formula |
|---|---|
Stopping distance ratio | |
Stopping time ratio |
◉ Bullet Through Planks:
Table 1: Bullet Special Cases
Condition | Result |
|---|---|
❖ Potential Energy:
◉ Definition: Energy stored due to configuration or position in a field
◉ Gravitational PE:
Table 1: Gravitational Potential Energy
Quantity | Formula |
|---|---|
◉ Special PE Formulae:
Table 1: Potential Energy Special Cases
Case | Increase in PE |
|---|---|
Elastic potential energy |
◉ Sign of PE:
- •Attractive forces → PE negative
- •Repulsive forces → PE positive
❖ Work-Energy Theorem:
◉ Statement: Work done on a body equals change in kinetic energy
◉ Formula:
◉ Applications:
Table 1: Work-Energy Applications
Case | Work done / Result |
|---|---|
Empty full tank to half depth | |
Take out all liquid from full tank | |
Released chain: velocity when end leaves edge | |
❖ Conservative and Non-conservative Forces:
Table 1: Conservative vs Non-conservative Forces
Feature | Conservative force | Non-conservative force |
|---|---|---|
Mechanical energy | Conserved | Not conserved |
Work done | Depends only on initial and final positions | Depends on actual path |
Closed path work | Zero | Not zero |
Examples | Gravitational, electrostatic, magnetostatic, all central forces | Frictional, viscous forces |
▢ Collision:
❖ Definition: Mutual interaction between particles for short time interval in which momentum and kinetic energy may change
❖ Law of Collision:
◉ Statement: Velocity of separation after collision is directly proportional to velocity of approach before collision
Table 1: Coefficient of Restitution
Quantity | Formula / Point |
|---|---|
Velocity of separation | |
Velocity of approach | |
Relation | |
Coefficient of restitution | |
Nature | Dimensionless and unitless |
Elastic collision | |
Perfectly inelastic collision | |
Practical collision |
◉ Notes:
- •Linear momentum is conserved in every collision
- •Total energy is conserved in every collision
- •Kinetic energy is conserved only in elastic collision
❖ Types of Collision:
Table 1: Elastic vs Inelastic Collision
Feature | Elastic collision | Inelastic collision |
|---|---|---|
Total energy | Conserved | Conserved |
Linear momentum | Conserved | Conserved |
Kinetic energy | Conserved | Not conserved |
Coefficient of restitution | ||
Perfectly inelastic collision | — |
❖ Elastic Collision in One Dimension:
◉ Momentum Conservation:
◉ Kinetic Energy Conservation:
◉ Final Velocities:
Table 1: Elastic Collision Final Velocities
Quantity | Formula |
|---|---|
◉ Special Cases:
Table 1: Elastic Collision Special Cases
Condition | Result |
|---|---|
❖ Inelastic Collision:
◉ Final Velocities with Coefficient e:
Table 1: Inelastic Collision Final Velocities
Quantity | Formula |
|---|---|
◉ Perfectly Inelastic Collision:
Table 1: Perfectly Inelastic Collision
Quantity | Formula / Point |
|---|---|
Bodies move with common velocity | |
Momentum equation | |
Common velocity | |
Coefficient of restitution | |
Loss in K.E. |
❖ Body Dropped and Rebounds:
◉ Condition:
Table 1: Rebound Formulae
Quantity | Formula |
|---|---|
Striking velocity | |
Velocity of bounce | |
Coefficient of restitution | |
❖ Oblique Elastic Collision:
◉ Condition:
Table 1: Oblique Collision Equations
Conservation | Equation |
|---|---|
Kinetic energy | |
Momentum along X-axis | |
Momentum along Y-axis |
◉ Special Case:
▢ Machines:
Table 1: Simple Machine Terms
Term | Formula |
|---|---|
Mechanical advantage / MA | |
Velocity ratio / VR | |
Efficiency | |
Relation |
▢ Read and Digest:
Table 1: Important Points
Fact | Point / Formula |
|---|---|
Flowing water | Has both K.E. and P.E. |
Potential energy | Exists only for conservative forces |
Energy change | Work is necessarily done |
Static/dynamic equilibrium | Net work done = 0 |
Unstable equilibrium | Potential energy maximum |
Air bubble rises in water | P.E. decreases because work is done by upthrust |
Force to hold machine gun | |
Oscillation | Occurs about stable equilibrium only |
Slope of work-time graph | |
Gravity work | Positive downward, negative upward |
Constant power motion | |
Hydrogen balloon in air | Weight is negative; gravitational P.E. decreases with altitude |
Like charges brought together | P.E. increases |
Unlike charges brought together | P.E. decreases |
Centripetal force | Power dissipated = 0 |
▢ High-Yield Recall:
Table 1: Work, Energy, Power and Collision One-Liners
Fact | Answer |
|---|---|
Work | |
Work nature | Scalar |
SI unit of work | Joule |
CGS unit of work | Erg |
Joule-erg relation | |
Work by centripetal force | Zero |
Work by friction | Negative |
Power | |
1 HP | |
Energy | Capacity to do work |
Kinetic energy | |
K.E. in terms of momentum | |
Momentum in terms of K.E. | |
Elastic P.E. | |
Work-energy theorem | |
Conservative force closed path work | Zero |
Conservative forces | Gravitational, electrostatic, magnetostatic, central forces |
Non-conservative forces | Frictional, viscous |
Collision | Short-time mutual interaction |
Coefficient of restitution | |
Elastic collision | |
Perfectly inelastic collision | |
Conserved in every collision | Linear momentum and total energy |
K.E. conserved only in | Elastic collision |
Equal masses elastic collision | Velocities exchange |
Perfectly inelastic common velocity | |
Loss in K.E. in perfectly inelastic collision | |
Rebound coefficient | |
Height after n bounces | |
Velocity after n bounces | |
Oblique elastic equal masses | Move perpendicular after collision |
Mechanical advantage | |
Velocity ratio | |
Efficiency |
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A car can be stopped over a distance x when its momentum is p. What will be the stopping distance when momentum is 2p?
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Q4.
If two bodies of masses 4M and 16M move with same kinetic energy, what is the ratio of their momentum?
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Q5.
'A' and 'B' are two bodies and A is lighter than B. If they have equal momentum, then the kinetic energy of A is:
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Q6.
If the product of mass and velocity is doubled, the new kinetic energy is how many times the original kinetic energy?
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Q7.
When momentum of a body is increased by 100%, its kinetic energy increases by:
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A train of mass 'm' is moving with velocity 'v' making an angle '6' with horizontal straight line power delivered is?
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Q10.
If kinetic energy changes by 4%, the momentum changes by approximately:
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Q11.
If a stone of mass 'M' dropped from height 'h' penetrates distance 's' into sand, the average resistance offered by the sand to the stone is:
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Q12.
What happens to the linear momentum of the projectile when its velocity is doubled?
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Q13.
A car is going with a linear momentum p. When brakes are applied, it comes to a stop in a distance s. If the same car were going with a linear momentum 2p and the brakes are applied (assume that the brake force is same in the two cases), it comes to a stop in a distance of:
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Q14.
For a constant power, the velocity of a body depends on displacement as:
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Q15.
A bullet of mass 10 g moving with a velocity 200 m/s hits a wooden block and penetrates 2 cm before coming to rest. What is its average force exerted on bullet during penetration?
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Q16.
If an object fall from top of inclined plane and get velocity 'u' in ground. How much distance will it cover if it is projected upward with that velocity?
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A person on a moving train throws upwards a coin, and if it falls behind him, then train is
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Q24.
The slope of a velocity- time graph gives
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A body cover 1/3 rd distance with V1, velocity next 2/3 rd distance with V2 velocity the average velocity.
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Q35.
Two stones A and B are thrown from the top of a tower. The stone A is thrown vertically upward while the stone B is thrown vertically downward with the same speed. Which one of the following statements is true?
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A racing car moving along circular track of radius R at constant speed v has described angle theta about centre of the track n certain time. What is the average velocity for the interval of time?
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If the displacement of a body is proportional to square of time. Then body has
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A person travels certain distance x due east at constant velocity v, and then he travels equal distance x due north at constant velocity v2. What is his average velocity for entire journey?
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Q56.
A person travels for certain time t due east at constant velocity v, and then he travels for equal time t due north at constant velocity v2. What is his average velocity for entire journey?
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In the above question if the car makes 'U' turn then average acceleration of the car will be
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A ball thrown vertically upward covers equal distances in its fourth and fifth second. Then initial velocity of projection will be
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A body is projected vertically upward from point A, the top of a tower. It reaches the ground in t1 secs. If it is projected vertically downwards from A with the same velocity, it reaches the ground in t2 secs. If it falls freely from A, it would reach the ground in
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A body falls freely from rest and has velocity v after it falls through a height h. The distance it has to fall down further for its velocity to become double is
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Two bodies are thrown vertically upward with their initial velocities in ratio 2: 3. Then the ratio of maximum heights attained by them is
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Q92.
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A body of mass 'm' is released from height 'h' in time 't'. Then, acceleration is determined by:
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