
I've attached the Lecture Notes to this video. Don't forget to download them!
Discover energy as a property of a system, focusing on mechanical energy with kinetic and potential forms, and learn that total energy is conserved and can transfer between forms.
Define work for a constant force as the dot product of force and displacement. Only the force component along the displacement contributes, so w = F cos theta Δx.
Explore the units of work from the work–kinetic energy relation, showing that work is a scalar with SI units joule (kg·m²/s²) and equals newton-meter.
Sum the work of each force to obtain the net work on an object; on a horizontal drag, gravity and the normal force do zero work.
Select a reference point for potential energy, then compute changes in gravitational potential energy and the work by gravity using height differences or force–displacement.
Apply conservation of mechanical energy to a platform diver from 10 m to 5 m, zero potential at ground; mass cancels, final speed equals sqrt(2 g times the height difference).
Apply conservation of energy: three balls thrown from a cliff with equal speed reach the ground with the same final speed, regardless of direction, because total mechanical energy is constant.
Apply the extended work energy theorem to a gravity–spring system, showing that the work by gravity and the spring equals changes in kinetic energy and total mechanical energy remains conserved.
apply conservation of energy to a 3 kg mass released from 5 m on a curved frictionless ramp with a 400 N/m spring, yielding x ≈ 0.86 m.
Analyze a 2.4 kg block dropped from five meters onto a spring, derive the spring constant from maximum compression, and find speed at 15 cm using energy conservation (no friction).
The lecture shows how gravity does negative work when moving a mass from the earth’s surface to three radii, with W = -2/3 GMm/R_E.
Explore power as the time rate of energy transfer, defined as work divided by the time interval, and examine how this expands the work-time relationship for constant forces.
Compute the minimum motor power to lift a fully loaded elevator at constant speed using a free-body diagram, accounting for weight and friction, then convert power to horsepower.
Practice nine multiple choice problems, mixing conceptual questions with small calculations, using the attached PTF to work before watching the solutions. Reach out with any questions via email or message.
Apply energy conservation to the pendulum: initial gravitational potential energy becomes final kinetic energy at the bottom. Compute height using 5 m rope and 53°, then v ≈ 6.3 m/s.
Compare two cases of pushing a crane on a horizontal floor: adding a child increases the normal force and kinetic friction, making w2 larger than w1 for the same displacement.
Practice nine multiple-choice energy problems, balancing conceptual questions with small calculations; download the problem set, work on the problems, then view the solutions.
Calculate the potential energy loss and power of a 50-meter waterfall with mass flow 5.5×10^6 kg s^-1, then convert to dollars per year using kilowatt-hour pricing.
Apply conservation of energy to a 2 kg book dropped from 10 m; calculate initial potential energy, final kinetic energy, and final speed of about 12.9 m/s.
Use conservation of energy on a frictionless roller coaster to compute speeds at A, B, C, D; v_B = 0, v_C = sqrt(g h), v_D = sqrt(2 g h).
The first part of this problem involves a bit of calculus. Part b) is more important where you are asked to apply the potential equation formula.
Apply conservation of energy to a 2 kg block dropped from 0.40 m onto a spring to find the maximum compression; solving the energy balance yields a 0.10 m compression.
Examine how dissipated energy from air resistance lowers height for a 9.4 kg mass; equate energy loss to m g delta y to show frictionless rise is 738 meters higher.
Apply the work-energy theorem to a rock sliding down a slope with friction, computing gravitational potential energy, frictional work, and the final speed using the normal force.
Apply the work-energy theorem to a two-block system connected by a string, accounting for constant gravity, friction, tension, and normal forces to find the final speed after distance L.
Parts (a) and (b) should be straightforward but part (c) is a little harder. Think about what it means for the strings to remain straight (taught).
Use energy conservation in a frictionless pulley with two masses and a spring on an incline to determine speeds of both blocks when the spring returns to unstretched length.
This comprehensive course covers kinetic energy, work, potential energy, and conservation of energy. The course combines lectures that summarize the important concepts and tutorials that will guide you and help you develop a problem-solving strategy. You'll learn how to apply conservation of energy principles to study the dynamics of systems.
Topics included in this class are:
1) Kinetic Energy, Work
2) Applying Work-Energy Theorem
3) Work done by gravitational forces, springs
4) Power
5) Potential Energy and Conservation of Mechanical Energy
The work-energy theorem is an extremely powerful technique use to solve physics problems.
There are over 40 fully solved problems ranging in difficulty. I've mixed in many conceptual problems as well as algebraic problems to help you practice applying energy principles to solve problems. You will notice that the problems start easy but build. By the end of the topic you'll be solving complex problems dealing with the concept of conservation of energy.
If at any point you don't understand something in my videos please feel free to reach out. I'm always willing to help someone learn. Physics Ninja always has your back!
Happy Learning and I hope you will truly enjoy this course.
Dr. E., Physics Ninja and Expert Physics and Math Teacher.