Work, Energy, and Power
Energy:
Definition: "Energy cannot be created or destroyed; it can only be changed from one form to another" —Albert Einstein.
Understanding energy is crucial to Physics; it permeates all branches of the subject.
Energy: An Overview
Definition: Energy is not easy to define; it varies based on force types (e.g., gravitational, elastic, thermal).
Law of Conservation of Energy:
Energy can’t appear or disappear in a closed system; it transforms from one form to another.
Work is the method of transferring energy across systems.
Work
Definition of Work:
Work (W) is done when a force (F) acts over a distance (d):
[ W = Fd ]
Work is a scalar quantity, can be positive, negative, or zero.
Units of Work:
Measured in Joules (J), where 1 Joule = 1 Newton-meter (N·m).
Calculating Work
Example 1:
Lifting a 2 kg book at constant velocity over 3 m:
Weight of book: [ F = mg = 20 N ]
Work done: [ W = Fd = (20 N)(3 m) = 60 J ]
Work at an Angle
Modified Formula:
For forces applied at an angle: [ W = Fd \cos(θ) ]
Example of a crate at 30° angle:
Work done on the crate requiring the angle component.
Examples of Work
Example 2:
Moving 15 kg crate across a horizontal surface at 30°:
[ W = (69 N \cdot \cos 30°)(10 m) = 600 J ]
Example 3:
Work by normal force is zero as it's perpendicular to displacement.
Friction does negative work, calculated as: [ W = -µk FN d = -462 J ]
Kinetic Energy
Definition: Energy of an object due to motion: [ K = mv^2 ]
Positive work increases kinetic energy.
Work–Energy Theorem
Energy transfer occurs through work, connecting kinetic energy changes to work done:
[ W = K_f - K_i ]
Example: Kinetic energy of a 0.1 kg ball at 30 m/s gives: [ K = 0.5 mv^2 ]
Potential Energy
Definition: Arises from an object's position eg. gravitational potential energy:
[ U = mgh ] (height relative to a reference point).
Example: Lifting mass to height has potential energy transformed into kinetic when falling.
Conservation of Mechanical Energy
Total mechanical energy remains constant when only conservative forces act:
[ K_i + U_i = K_f + U_f ]
Example: Ball at height 5 m has potential energy that changes to kinetic energy.
Work Done by Non-Conservative Forces
When dealing with non-conservative forces (e.g., friction):
Adjusted equation: [ K_i + U_i + W_{other} = K_f + U_f ]
Power
Definition: Power is the rate of doing work: [ P = \frac{W}{t} ]
Units: Watts (W), where 1 W = 1 J/s.
Example: Moving a crate with 300 N force over 6 m in 20 s gives power output of 90 W.
Summary
Work is the application of force across a displacement, resulting in energy changes.
Energy is conserved in a closed system; total initial equals total final energy.
The power output defines how quickly work is done, measured in watts.
Work, Energy, and Power
Energy:
Definition: "Energy cannot be created or destroyed; it can only be changed from one form to another" —Albert Einstein.
Understanding energy is crucial to Physics; it permeates all branches of the subject.
Energy: An Overview
Definition: Energy is not easy to define; it varies based on force types (e.g., gravitational, elastic, thermal).
Law of Conservation of Energy:
Energy can’t appear or disappear in a closed system; it transforms from one form to another.
Work is the method of transferring energy across systems.
Work
Definition of Work:
Work (W) is done when a force (F) acts over a distance (d):
[ W = Fd ]
Work is a scalar quantity, can be positive, negative, or zero.
Units of Work:
Measured in Joules (J), where 1 Joule = 1 Newton-meter (N·m).
Calculating Work
Example 1:
Lifting a 2 kg book at constant velocity over 3 m:
Weight of book: [ F = mg = 20 N ]
Work done: [ W = Fd = (20 N)(3 m) = 60 J ]
Work at an Angle
Modified Formula:
For forces applied at an angle: [ W = Fd \cos(θ) ]
Example of a crate at 30° angle:
Work done on the crate requiring the angle component.
Examples of Work
Example 2:
Moving 15 kg crate across a horizontal surface at 30°:
[ W = (69 N \cdot \cos 30°)(10 m) = 600 J ]
Example 3:
Work by normal force is zero as it's perpendicular to displacement.
Friction does negative work, calculated as: [ W = -µk FN d = -462 J ]
Kinetic Energy
Definition: Energy of an object due to motion: [ K = mv^2 ]
Positive work increases kinetic energy.
Work–Energy Theorem
Energy transfer occurs through work, connecting kinetic energy changes to work done:
[ W = K_f - K_i ]
Example: Kinetic energy of a 0.1 kg ball at 30 m/s gives: [ K = 0.5 mv^2 ]
Potential Energy
Definition: Arises from an object's position eg. gravitational potential energy:
[ U = mgh ] (height relative to a reference point).
Example: Lifting mass to height has potential energy transformed into kinetic when falling.
Conservation of Mechanical Energy
Total mechanical energy remains constant when only conservative forces act:
[ K_i + U_i = K_f + U_f ]
Example: Ball at height 5 m has potential energy that changes to kinetic energy.
Work Done by Non-Conservative Forces
When dealing with non-conservative forces (e.g., friction):
Adjusted equation: [ K_i + U_i + W_{other} = K_f + U_f ]
Power
Definition: Power is the rate of doing work: [ P = \frac{W}{t} ]
Units: Watts (W), where 1 W = 1 J/s.
Example: Moving a crate with 300 N force over 6 m in 20 s gives power output of 90 W.
Summary
Work is the application of force across a displacement, resulting in energy changes.
Energy is conserved in a closed system; total initial equals total final energy.
The power output defines how quickly work is done, measured in watts.