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SHM Fundamentals

A comprehensive introduction to Simple Harmonic Motion, covering restoring forces, kinematics, and energy conservation in oscillating systems.

CMChuguna Murugesan

SHM Fundamentals

A comprehensive introduction to Simple Harmonic Motion, covering restoring forces, kinematics, and energy conservation in oscillating systems.

CMChuguna Murugesan
  • Period: Independent of mass; depends on Length (L).
  • Pendulum Cycle

    \( U_g \leftrightarrow K \)

    Spring Cycle

    \( U_s \leftrightarrow K \)

    05A

    Matrix: Mass-Spring System

    Compressed

    Equilibrium

    Extended

    Mass-Spring Dynamics mapping Work Area

    VariableCompressedEquilibriumExtended
    Displacement (x)
    Net Force (\(F_{net}\))
    Acceleration (\(a\))
    Velocity (\(v\))
    Potential (\(U_s\))
    Kinetic (\(K\))
    Total Energy (\(E\))

    05B

    Matrix: Simple Pendulum Profile

    Left Peak

    Equilibrium

    Right Peak

    Angular Dynamics Profile Identify variable states

    VariableLeft PeakEquilibriumRight Peak
    Angular Disp. (\(\theta\))
    Restoring Force (\(F_{res}\))
    Acceleration (\(a\))
    Velocity (\(v\))
    Grav. Potential (\(U_g\))
    Kinetic Energy (\(K\))
    Total Energy (\(E\))

    Dynamics Mastery Profile Completed

    Discussion Prompts

    "If we moved this entire spring system to the moon, would the period change? Why or why not?" (Answer: No, period depends on mass and stiffness, not local gravity.)

    "How does the behavior of a 'stiff' spring (large k) compare to a 'loose' spring (small k) in terms of timing and energy?"

    Potential Energy
    Show your algebraic derivation.

    10. Graph Interpretation: Sketch a rough Force vs. Displacement graph for two springs: one with constant \( k \) and one with constant \( 2k \). Explain how the slopes of these graphs relate to the "stiffness" of the systems.

    11. Pendulum Condition: Justify the requirement that a simple pendulum’s angle must remain small (\( < 15^\circ \)) to be considered Simple Harmonic Motion. What happens to the "restoring force" if the angle is too large?

    12. Conservation Claim: A student claims that for a vertical spring, "Total Energy is conserved only if you pull the mass down from equilibrium." Refute or support this claim using the Law of Conservation of Energy.

    Mastery Quest Validated

    Page 3 of 3

    \[ E_{total} = K + U \]

    Total energy remains the same throughout every cycle.

    Max K At Equilibrium

    Max U At Amplitude

    The SHM Pulse Check

    StateForce (F)Velocity (v)Accel (a)Energy
    EquilibriumZeroMAXZeroAll Kinetic
    AmplitudeMAXZeroMAXAll Potential

    Kinematic Time-Profiles

    1. Displacement vs. Time

    Typically modeled as a cosine function starting at amplitude \( A \). The period \( T \) is the time between successive peaks.

    \[ x(t) = A\cos(\omega t) \]

    where \( \omega = 2\pi f = 2\pi/T \) is angular frequency.

    Position (x) Time (t)

    2. Velocity vs. Time

    Velocity is the derivative (slope) of position. It is 90° out of phase. When \( x=0 \), \( v \) is at its maximum magnitude.

    \[ v(t) = -A\omega\sin(\omega t) \]

    \[ v_{max} = A\omega = A\sqrt{\frac{k}{m}} \]

    3. Acceleration vs. Time

    Acceleration is the derivative of velocity. It is 180° out of phase with position—effectively its mirror image.

    \[ a(t) = -A\omega^2\cos(\omega t) \]

    \[ a_{max} = A\omega^2 = \frac{kA}{m} \]

    AP Question Pattern: Amplitude Impact

    "If Amplitude is doubled, what happens to..."

    • Period: No Change (Linearity).
    • Max Force: Doubles (\( F \propto A \)).
    • Max Velocity: Doubles (\( v \propto A \)).
    • Max Acceleration: Doubles (\( a \propto A \)).
    • Total Energy: Quadruples (\( E \propto A^2 \)).

    Remember: SHM requires the period to be amplitude-independent. If the period changes with amplitude in an AP FRQ, the spring is not linear, and the system is not Simple Harmonic.

    Physics Advanced Studies Series Topic 7 Reference

    0s1s2s3s4s5s6s7s8s

    +\(F_{max}\) -\(F_{max}\)

    Page 2 of 4 // Synthesis Challenge A

    Section II: Waveform Synthesis (Energy)

    10. Derive: Potential Energy (\(U_s\)) vs. Time (t)

    0s1s2s3s4s5s6s7s8s

    Max \(U_s\) 0

    11. Derive: Kinetic Energy (K) vs. Time (t)

    0s1s2s3s4s5s6s7s8s

    Max \(K\) 0

    12. Derive: Total Mechanical Energy (\(E_{tot}\)) vs. Time (t)

    0s1s2s3s4s5s6s7s8s

    Total Energy 0

    Page 3 of 4 // Synthesis Challenge B

    Section III: Quantitative Synthesis

    Physical Parameters for Section II & III:

    Mass (m) 2.0 kg

    Period (T) 4.0 s

    Amplitude (A) 2.0 m

    13. Calculate the spring constant \(k\) for the oscillator in Section II.

    14. Determine the Maximum Speed (\(v_{max}\)) reached by the mass.

    15. Predict: If the mass were doubled, but the spring constant remained fixed, calculate the new Period.

    Final Submission Verified // AP Physics 1

    Visualizing the Cycle

    Section 03: Graphical Analysis

    The Time-Evolution Profiles

    Position (x)

    \( \cos \)

    Starts at peak (+A). Velocity is the slope here (starts at zero).

    Velocity (v)

    \( -\sin \)

    Peaks when position is zero. This is the 90° phase shift.

    Acceleration (a)

    \( -\cos \)

    Mirrors position. When position is max positive, acceleration is max negative.

    Amplitude Scaling Logic

    Changing the Amplitude (A) impacts nearly every variable in the system EXCEPT the frequency and period.

    Max Force \( F_{max} \propto A^1 \)

    Max Velocity \( v_{max} \propto A^1 \)

    Total Energy \( E_{tot} \propto A^2 \)

    Pro-Tip: If an FRQ asks you to double the amplitude, your velocity should double, but your energy bar charts should grow four times higher.

    Critical Check

    Is the system Simple Harmonic? Use this checklist:

    • The net force acts toward equilibrium (\( - \)).
    • The force is linear (\( x^1 \)).
    • The period is amplitude-independent.
    • The motion can be modeled as a sine/cosine wave.

    AP Physics 1 Dynamic Reference Unit 7.1 / 7.4

    Increase \( k \)? System speeds up

    © Physics Visual reference series Conceptual Mastery Guide

    Continuous Energy Waveforms

    Total Energy (E)

    Time Evolution →

    Potential Energy (U): Max at amplitudes; zero at equilibrium.

    Kinetic Energy (K): Max at equilibrium; zero at amplitudes.

    Energy is always positive (\( K = \frac{1}{2}mv^2 \), \( U = \frac{1}{2}kx^2 \)) and oscillates at twice the frequency of displacement.

    AP Physics Mastery Guide Topic 7 Reference Final

    Total Energy (E)

    Time →

    Potential Energy (U)

    Kinetic Energy (K)

    Energy waves are always positive and oscillate at twice the frequency of displacement.

    AP Physics Mastery Reference Topic 7.1 / 7.4 Final

    T/2

    3T/4

    T

    Time (t) →

    Graph 03: Acceleration (a) vs. Time

    +\(a_{max}\) -\(a_{max}\)

    0

    T/4

    T/2

    3T/4

    T

    Time (t) →

    Graph 04: Potential Energy (U) vs. Time

    \(U_{max}\) 0

    0

    T/4

    T/2

    3T/4

    T

    Time (t) →

    Graph 05: Kinetic Energy (K) vs. Time

    \(K_{max}\) 0

    0

    T/4

    T/2

    3T/4

    T

    Time (t) →

    Graph 06: Total Mechanical Energy (E) vs. Time

    \(E_{tot}\) 0

    0

    T/4

    T/2

    3T/4

    T

    Time (t) →

    0T/4T/23T/4T

    \(E_{tot}\) 0

    Time (t) →

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