Detailed Study Notes on Energy Conservation Concepts and Calculations

LESSON 5.1 - Potential Energy (PE), Kinetic Energy (KE), and Total Mechanical Energy (TME)

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  • Key equations:

    • Potential Energy (PE):
      U1=mgyU_1 = mgy

    • Where:

      • $U_1$: potential energy (Joules or J)

      • $m$: mass (kilograms or kg)

      • $g$: acceleration due to gravity ($9.8 ext{ m/s}^2$)

      • $y$: height (meters or m)

    • Kinetic Energy (KE):
      K=rac12mv2K = rac{1}{2}mv^2

    • Where:

      • $K$: kinetic energy (J)

      • $m$: mass (kg)

      • $v$: velocity (meters per second or m/s)

  • Energy transformations:

    • From point 1 to 2, energy converts from potential to kinetic.

    • From point 4 to 5, energy also transforms, confirming the conversion.

    • Position 3 has more potential energy than position 5 because it is at a greater height.

    • Position 4 has the greatest kinetic energy, typically the lowest point in a height differential.

Schedule for Current Lesson (1/22/2026)

  • Due Today: Popper Lab

  • Objectives:

    1. Notes on Mechanical Energy.

    2. Discuss Energy Conservation.

    3. Work through examples of KE to PE transformations.

  • Assignments/Announcements:

    1. Complete the lab part started previously.

    2. If it is an e-Day (Monday), expect assignments from Pearson Practice 5.1.

  • Goal:

    • Investigate conservation of energy examples related to kinetic and potential energy transforms.

    • Utilize Pear Deck for interactive learning.

Law of Conservation of Energy

  • Statement: The law of conservation of energy asserts that:

    • Energy cannot be created or destroyed; it can only be transformed from one form to another.

  • Types of energy involved:

    • Kinetic Energy (KE)

    • Potential Energy (PE)

    • Total Mechanical Energy (TME)

  • Example Inputs:

    • Height: $0.40 ext{ m}$

    • Speed: $0.00 ext{ m/s}$

Conservation of Energy

  • Energy Measurement:

    • Energy is measured in Joules (J).

  • Types of Mechanical Energy:

    1. Potential Energy (Stored Energy):

    • Gravitational potential energy described by the formula: U1=mgyU_1 = mgy

      • Where:

        • $m$: mass (kg)

        • $g$: acceleration due to gravity ($9.8 ext{ m/s}^2$)

        • $y$: height (m)

    1. Kinetic Energy (Energy of Motion):

    • Translational kinetic energy defined by: K=rac12mv2K = rac{1}{2} mv^2

      • Where:

        • $m$: mass (kg)

        • $v$: velocity (cm/s)

    • Rotational kinetic energy defined as: Kw=rac12Iheta2K_w = rac{1}{2} I heta^2

      • Where:

        • $K_w$: rotational kinetic energy (J)

        • $I$: moment of inertia

        • $ heta$: angular velocity

Conservation of Energy Principle

  • The Total Mechanical Energy (TME) is conserved in an isolated system:
    TME<em>1=TME</em>2TME<em>1 = TME</em>2</p></li><li><p>Thetotalmechanicalenergyincludesbothpotentialandkineticenergyandisgivenby:<br></p></li><li><p>The total mechanical energy includes both potential and kinetic energy and is given by:<br>TME = PE + KE</p></li><li><p>Thistotalisconstant,indicatingenergystoredaspotentialcanconverttokineticenergyinmotion,andviceversawithoutanylossduringthetransformation.</p></li></ul><h4id="2cdb216ccfa641beafb16956ada5988d"datatocid="2cdb216ccfa641beafb16956ada5988d"collapsed="false"seolevelmigrated="true">ConservationofEnergyMathConcepts</h4><ul><li><p>Commonscenariosinenergyproblemsinclude:</p><ol><li><p>StartingwithPotentialEnergy(PE,stationarymassatheight)whereitfallstoconverttoKineticEnergy:</p></li></ol><ul><li><p></p></li><li><p>This total is constant, indicating energy stored as potential can convert to kinetic energy in motion, and vice versa without any loss during the transformation.</p></li></ul><h4 id="2cdb216c-cfa6-41be-afb1-6956ada5988d" data-toc-id="2cdb216c-cfa6-41be-afb1-6956ada5988d" collapsed="false" seolevelmigrated="true">Conservation of Energy Math Concepts</h4><ul><li><p>Common scenarios in energy problems include:</p><ol><li><p>Starting with Potential Energy (PE, stationary mass at height) where it falls to convert to Kinetic Energy:</p></li></ol><ul><li><p>PE1 = KE2</p></li><li><p></p></li><li><p>mgh_1 = rac{1}{2} mv^2</p></li></ul><ol><li><p>StartingwithKineticEnergy(movingobject)thatascends,convertingtoPotentialEnergy:</p></li></ol><ul><li><p></p></li></ul><ol><li><p>Starting with Kinetic Energy (moving object) that ascends, converting to Potential Energy:</p></li></ol><ul><li><p>KE1 = PE2</p></li><li><p></p></li><li><p> rac{1}{2} m v_1^2 = mgh</p></li></ul></li></ul><h4id="24d1d1cc99d44851a57b75f0b15658d8"datatocid="24d1d1cc99d44851a57b75f0b15658d8"collapsed="false"seolevelmigrated="true">GroupPractice(CaseStudy:Skier)</h4><ul><li><p>Scenario:A65kgskierstartsfromrestatthetopofan80mtallhillandskisdown.</p><ol><li><p>Calculatethespeedatthebottomofthehill.</p></li></ol><ul><li><p>Usethepotentialenergyatthetop:<br></p></li></ul></li></ul><h4 id="24d1d1cc-99d4-4851-a57b-75f0b15658d8" data-toc-id="24d1d1cc-99d4-4851-a57b-75f0b15658d8" collapsed="false" seolevelmigrated="true">Group Practice (Case Study: Skier)</h4><ul><li><p>Scenario: A 65 kg skier starts from rest at the top of an 80 m tall hill and skis down.</p><ol><li><p>Calculate the speed at the bottom of the hill.</p></li></ol><ul><li><p>Use the potential energy at the top: <br>PE = mgh = (65 ext{ kg})(9.8 ext{ m/s}^2)(80 ext{ m}) = 50,960 ext{ J}</p></li><li><p>Equatetokineticenergyatthebottom:</p></li><li><p>Equate to kinetic energy at the bottom:KE = rac{1}{2} mv^2 ightarrow 50,960 = rac{1}{2}(65)v^2

    • Solve for $v$:

    • v^2 = rac{50,960 imes 2}{65}
      ightarrow v^2 = 1,568
      ightarrow v = 40 ext{ m/s}$$

Additional Group Practice

  • A pendulum ball with a mass of 0.3 kg swings from rest at point A to point E without any work done. Calculating each state:

    • Point A:

    • PE = $mgh = (0.3)(9.8)(0.5) = 1.47 ext{ J}$,

    • KE = $0 ext{ J}$,

    • ME at point A = $1.47 ext{ J}$.

    • Point E (lower position):

    • PE = $0 ext{ J}$,

    • KE = Calculate using $KE = ME - PE
      ightarrow KE = 1.47 ext{ J}$.

    • The velocity ($v$) can also be calculated using the energy relations.

  • Conservation of Mechanical Energy will apply throughout the motion from point A to point B and beyond, ensuring the total mechanical energy remains equal at all points during the pendulum's swing.