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    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/General_Physics_I%3A_Classical_Mechanics/26%3A_Energy/26.02%3A_Potential_Energy
      1h+R=1RhR2+h2R3h3R4+ \[U(h) =G M_{\oplus} m\left[\frac{1}{R_{\oplus}}-\left(\frac{1...1h+R=1RhR2+h2R3h3R4+ U(h)=GMm[1R(1RhR2+h2R3h3R4+)]
    • https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Physics_I_(2211)/11%3A_Oscillations/11.02%3A_Energy_in_Simple_Harmonic_Motion
      Figure \PageIndex1: The transformation of energy in SHM for an object attached to a spring on a frictionless surface. (a) When the mass is at the position x = + A, all the energy is stored as po...Figure \PageIndex1: The transformation of energy in SHM for an object attached to a spring on a frictionless surface. (a) When the mass is at the position x = + A, all the energy is stored as potential energy in the spring U = 12kA 2 . The kinetic energy is equal to zero because the velocity of the mass is zero. (b) As the mass moves toward x = −A, the mass crosses the position x = 0.
    • https://phys.libretexts.org/Bookshelves/University_Physics/Physics_(Boundless)/15%3A_Waves_and_Vibrations/15.3%3A_Periodic_Motion
      The period is the duration of one cycle in a repeating event, while the frequency is the number of cycles per unit time.
    • https://phys.libretexts.org/Bookshelves/College_Physics/College_Physics_1e_(OpenStax)/16%3A_Oscillatory_Motion_and_Waves/16.01%3A_Hookes_Law_-_Stress_and_Strain_Revisited
      An oscillation is a back and forth motion of an object between two points of deformation. An oscillation may create a wave, which is a disturbance that propagates from where it was created. The simple...An oscillation is a back and forth motion of an object between two points of deformation. An oscillation may create a wave, which is a disturbance that propagates from where it was created. The simplest type of oscillations and waves are related to systems that can be described by Hooke’s law.
    • https://phys.libretexts.org/Bookshelves/University_Physics/University_Physics_(OpenStax)/Book%3A_University_Physics_I_-_Mechanics_Sound_Oscillations_and_Waves_(OpenStax)/15%3A_Oscillations/15.03%3A_Energy_in_Simple_Harmonic_Motion
      The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is ...The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is the force constant of the system. Elastic potential energy stored in the deformation of a system can be described by Hooke’s law as U = (1/2)kx^2. Energy in the simple harmonic oscillator is shared between elastic potential energy and kinetic energy, with the total being constant.
    • https://phys.libretexts.org/Courses/Muhlenberg_College/MC_%3A_Physics_213_-_Modern_Physics/02%3A_Waves/2.03%3A_Energy_in_Simple_Harmonic_Motion
      The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is ...The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is the force constant of the system. Elastic potential energy stored in the deformation of a system can be described by Hooke’s law as U = (1/2)kx^2. Energy in the simple harmonic oscillator is shared between elastic potential energy and kinetic energy, with the total being constant.
    • https://phys.libretexts.org/Courses/Muhlenberg_College/Physics_122%3A_General_Physics_II_(Collett)/15%3A_Oscillations/15.03%3A_Energy_in_Simple_Harmonic_Motion
      The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is ...The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is the force constant of the system. Elastic potential energy stored in the deformation of a system can be described by Hooke’s law as U = (1/2)kx^2. Energy in the simple harmonic oscillator is shared between elastic potential energy and kinetic energy, with the total being constant.
    • https://phys.libretexts.org/Workbench/PH_245_Textbook_V2/14%3A_Oscillations/14.03%3A_Energy_in_Simple_Harmonic_Motion
      The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is ...The simplest type of oscillations are related to systems that can be described by Hooke’s law, F = −kx, where F is the restoring force, x is the displacement from equilibrium or deformation, and k is the force constant of the system. Elastic potential energy stored in the deformation of a system can be described by Hooke’s law as U = (1/2)kx^2. Energy in the simple harmonic oscillator is shared between elastic potential energy and kinetic energy, with the total being constant.
    • https://phys.libretexts.org/Courses/Joliet_Junior_College/JJC_-_PHYS_110/05%3A_Book-_Physics_(Boundless)/5.08%3A_Waves_and_Vibrations/5.8.03%3A_Periodic_Motion
      The period is the duration of one cycle in a repeating event, while the frequency is the number of cycles per unit time.
    • https://phys.libretexts.org/Courses/Prince_Georges_Community_College/PHY_2040%3A_General_Physics_III/01%3A_Waves_and_Vibrations/1.3%3A_Periodic_Motion
      The period is the duration of one cycle in a repeating event, while the frequency is the number of cycles per unit time.

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