Kinetic vs. Potential Energy
Kinetic vs. Potential Energy: Physics 111 Notes
Theory & Concepts
Mechanical Energy: The total energy (kinetic + potential) in a system.
Kinetic Energy (KE): Energy associated with motion.
Parameters:
Formula:
KE=rac12mv2
Potential Energy (PE): Energy stored based on an object's position.
Parameters:
Types of Potential Energy:
Gravitational Potential Energy (GPE):
Formula:
PEg=mgh
Elastic Potential Energy (SPE):
Stored in springs.
Formula: PEs=rac12kx2
Electric Potential Energy: Related to positions of charged particles.
Work-Energy Theorem: Connects work done on an object to its kinetic energy change.
Non-conservative Forces: Forces like friction which transform mechanical energy into other forms (e.g., heat).
Include non-conservative work in the theorem:
W<em>net+W</em>c=riangleKE
Where $W_c$ is work done by non-conservative forces.
} mv^2 </p></li></ul></li></ul><h4id="f652910d−1dce−4908−b244−987c7b60d789"data−toc−id="f652910d−1dce−4908−b244−987c7b60d789"collapsed="false"seolevelmigrated="true">Work−EnergyTheorem</h4><ul><li><p><strong>ScalarQuantity</strong>:</p><ul><li><p>KineticenergyismeasuredinJoules(J).</p></li><li><p><strong>Work−EnergyTheoremStatement</strong>:</p></li><li><p>Thenetworkonanobjectisequaltothechangeintheobject′skineticenergy.</p></li><li><p>Importanttoconsidernonconservativeforces:<br> W{net} + W{c} = riangle KE </p></li><li><p>Whenfrictionispresent,adjusttheequationaccordingly:<br> W{net} = KEf - KE_i </p></li></ul></li></ul><h4id="1d3b78ab−b23d−45c8−b1e0−cfd2fbb1506e"data−toc−id="1d3b78ab−b23d−45c8−b1e0−cfd2fbb1506e"collapsed="false"seolevelmigrated="true">GravitationalPotentialEnergy</h4><ul><li><p><strong>Conceptualization</strong>:</p><ul><li><p>Potentialenergy(PE)asasystemproperty,especiallyinrelationtogravitationalforcesactingonobjects.</p></li><li><p>Updatethework−energytheoremtoincludegravitationalpotentialenergy:</p></li><li><p>Whendealingwithgravitationalwork:<br> Wg = F ext{cos}( heta) = mg(yi - y_f) ext{cos}(0°) </p></li><li><p>Incorporatemodificationswhenapplyingnon−conservativeforcesleadingtooverallmechanicalenergychanges:<br> W{net} = W{net} + W_g = riangle KE </p></li></ul></li></ul><h4id="408ec461−7105−4d63−a285−337ea05eefb6"data−toc−id="408ec461−7105−4d63−a285−337ea05eefb6"collapsed="false"seolevelmigrated="true">ConservationofMechanicalEnergy</h4><ul><li><p><strong>ConservativeForceDefinition</strong>:Pressure/forcesthatbehaveindependentlyofthepathtaken.</p></li><li><p><strong>KeyConcepts</strong>:</p><ul><li><p>Workdonethroughaclosedpathleadstozerochangeinenergy:<br> riangle MME = 0 </p></li><li><p>Mechanicalenergyconservationrelationship:<br> W_{net} = riangle KE + riangle PE
Where total mechanical energy $ riangle MME = KEf + PEf - (KEi + PEi)$ remains constant.
Elastic Potential Energy
Spring Mechanics:
The strength of the spring's bounce-back relates to its compression, signifying increased potential energy.
Hooke's Law: States that restoring force of the spring, $F_s$, is proportional to the displacement from its rest position:
F_s = -kx </p></li><li><p><strong>Work−EnergyRelation</strong>:</p></li><li><p>Averagespringforceimpactsworkdoneoveradistance:<br> W_s = rac{1}{2}kx^2 </p></li><li><p>Thepotentialenergyinthespringisdefinedas:<br> PE_s = rac{1}{2} kx^2 $$
Problem-Solving Approach
Steps:
Read and elucidate the question.
Define starting conditions and set a point of reference for conservation of energy.
Write the conservation equation while identifying unknowns.
Solve for the unknown value(s).