Forced vibrations and resonance (A-level only) — AQA A-Level Physics
Teaching note checked against the official specification.
Forced vibrations occur when a system is driven by an external periodic force, causing it to oscillate at the driving frequency rather than its natural frequency. Resonance is the dramatic increase in amplitude that occurs when the driving frequency matches the natural frequency of the system, a phenomenon with important applications and dangers in engineering and physics.
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Forced vibrations and resonance (A-level only) explained
Forced vibrations and resonance (A-level only) covers 3 specification points, including Qualitative treatment of free and forced… and Resonance and the effects of damping on the….
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Open a point below for its explanation and revision guidance.
Qualitative treatment of free and forced vibrations.
A free vibration occurs when an object oscillates at its natural frequency after being displaced, with no periodic external force. A forced vibration occurs when a periodic driving force makes the object oscillate at the driving frequency. At low driving frequencies the amplitude is small; as the driving frequency approaches the natural frequency the amplitude increases, reaching a maximum at resonance. The sharpness of the resonance curve depends on damping: heavier damping lowers and broadens the peak. You should describe these effects qualitatively, using examples such as a child on a swing pushed at the right moments, or a glass vibrating strongly when a sound wave matches its natural frequency.
Resonance and the effects of damping on the sharpness of resonance.
Resonance occurs when a system is driven at a frequency matching one of its natural frequencies, so energy transfer from the driver is maximised and amplitude peaks. The driver supplies energy each cycle; near resonance the system absorbs it efficiently, while away from resonance the response falls. Damping removes energy each cycle, so the amplitude peak is lower and broader. Light damping gives a tall, narrow resonance curve: the response is sharply tuned to the driving frequency. Heavy damping gives a low, wide curve, so the system responds over a wider frequency range but with smaller amplitude. The sharpness of resonance is therefore a measure of how narrow the peak is, often compared using the width of the curve at a chosen fraction of the peak amplitude. A useful method is to plot amplitude against driving frequency for several damping values and compare peak heights and widths.
Examples of these effects in mechanical systems and situations involving stationary waves.
Resonance and damping appear in many mechanical systems and in stationary-wave situations. A child on a swing pushed at the natural frequency builds a large amplitude; friction and air resistance damp it. A car suspension oscillates after a bump, and shock absorbers add damping to reduce the sharpness of resonance and settle the ride. A building or bridge can resonate when driven near a natural frequency, so dampers may be fitted. In stationary waves, resonance occurs when a system supports a standing-wave pattern at particular frequencies. A string fixed at both ends resonates when its length fits a whole number of half-wavelengths, and a tube can resonate at frequencies set by its boundary conditions. Damping broadens the response, so the resonant frequencies are less sharply defined and the stationary-wave amplitude is reduced.
Your focus
- Distinguish between free and forced vibrations using correct frequency terminology.
- Describe how amplitude varies with driving frequency and identify the resonance condition.
- Explain qualitatively how damping affects the resonance peak.
Show all 9 objectives
- Describe resonance as the condition where driving frequency matches a natural frequency and explain the resulting maximum energy transfer.
- Explain how increasing damping lowers and broadens the resonance peak, reducing the sharpness of resonance.
- Compare resonance curves for different amounts of damping using peak height and peak width.
- Describe examples of resonance and damping in mechanical systems, identifying the driver and the oscillating system.
- Explain how stationary waves form at resonant frequencies in strings and tubes using nodes, antinodes and boundary conditions.
- Explain how damping affects the amplitude and sharpness of resonance in stationary-wave situations.
Which command word is this?
Give a precise, formal statement of the term. For resonance, state that it is the condition when the driving frequency equals the natural frequency, resulting in maximum amplitude. No explanation required unless asked.
Forced vibrations and resonance (A-level only) exam tips
Topic Overview
Forced vibrations and resonance are key topics in A-level Physics that explore how systems respond to external periodic forces. Unlike free vibrations, where a system oscillates at its natural frequency, forced vibrations occur when an external driving force dictates the frequency of oscillation. This topic is crucial for understanding real-world phenomena such as musical instruments, engineering structures, and electrical circuits.
Resonance, a special case of forced vibration, occurs when the driving frequency matches the natural frequency, leading to a dramatic increase in amplitude. This concept is fundamental in physics and engineering, with applications ranging from tuning radios to designing earthquake-resistant buildings. Mastering this topic requires a solid grasp of energy transfer, damping, and the mathematical relationships governing oscillatory motion.
Key Concepts
- →Forced vibrations: The system oscillates at the driving frequency, not its natural frequency. The amplitude depends on the driving frequency and the amount of damping.
- →Resonance: Occurs when driving frequency equals natural frequency. The amplitude reaches a maximum, and energy transfer from the driver to the oscillator is most efficient.
- →Damping: Reduces the amplitude of resonance and broadens the resonance peak. Heavier damping results in a lower and wider peak; lighter damping gives a sharper, taller peak.
- →Phase relationship: At resonance, the driving force is in phase with the velocity of the oscillator (phase difference between force and displacement is 90 degrees).
- →Natural frequency: The frequency at which a system oscillates freely without any external force, determined by its physical properties (e.g., mass and stiffness).
Marking Points
- Distinguishes free vibration, where the system oscillates at its natural frequency, from forced vibration, where a periodic driving force determines the frequency.
- States that the amplitude of a forced vibration depends on the difference between the driving frequency and the natural frequency.
- Describes resonance as the condition where driving frequency equals natural frequency and amplitude reaches a maximum.
- Explains that increased damping reduces the maximum amplitude and broadens the resonance peak.
- Applies the ideas to a named example, such as a swing pushed at its natural frequency or a building vibrating in an earthquake.
- Resonance is the condition where the driving frequency equals a natural frequency of the system, giving maximum energy transfer per cycle and a maximum steady-state amplitude.
- At resonance the phase relationship between driver and oscillator is such that the driver does work on the system throughout the cycle, so energy input is greatest.
- Damping dissipates mechanical energy, usually as thermal energy, so the resonant amplitude is reduced compared with the undamped or lightly damped case.
- Increasing damping broadens the resonance curve, reducing the sharpness of resonance; decreasing damping narrows the curve and raises the peak.
- The sharpness of resonance can be compared by measuring the width of the resonance peak at a stated level, for example at half the peak amplitude, and relating a narrower width to sharper tuning.
- Practical examples include a mass on a spring driven by a vibrating support, a pendulum driven by a motor, or a loudspeaker cone near its natural frequency.
- A mechanical example must identify the driver, the oscillating system, and the natural frequency that is matched or approached.
- Damping in a mechanical system removes energy from the oscillations, often as thermal energy, so amplitudes decay or steady-state amplitudes are reduced.
- In stationary waves on a string fixed at both ends, resonance occurs at frequencies where the string length equals a whole number of half-wavelengths.
- In tubes, the resonant frequencies depend on whether the ends are open or closed, because the boundary conditions determine the allowed stationary-wave patterns.
- Damping broadens each resonance, so the stationary-wave response is less sharply tuned to a single driving frequency.
- A suitable comparison is a lightly damped and heavily damped system driven through the same frequency range, noting the change in peak height and width.
Examiner Tips
- 💡Use the terms driving frequency and natural frequency precisely in your answer.
- 💡Sketch or describe the amplitude–frequency graph, marking the peak at the natural frequency.
- 💡Link each statement to a familiar example so the qualitative explanation is clear.
- 💡Sketch two resonance curves on the same axes, one lightly damped and one heavily damped, and label peak height and width clearly.
- 💡Use the phrase sharpness of resonance only after defining what is being compared, such as the width of the peak at a stated amplitude level.
- 💡When explaining energy transfer, refer to the driver doing work on the oscillating system each cycle rather than saying energy is created.
- 💡Link any practical example back to the driving frequency and the natural frequency of the system, not just to large vibrations.
- 💡For each example, state the driver, the oscillating object, and why the driving frequency is near a natural frequency.
- 💡When discussing stationary waves, sketch the mode shape and mark nodes and antinodes before doing any calculation.
- 💡Use the same axes for comparing damped and undamped cases so the change in peak height and width is visible.
- 💡Keep explanations of damping tied to energy removal rather than to vague ideas of friction slowing everything down.
- 💡Always specify that in forced vibrations, the frequency of oscillation equals the driving frequency, not the natural frequency. This is a common mark lost in definitions.
- 💡When describing resonance, mention that the amplitude is maximum and that this occurs when driving frequency equals natural frequency. Include the effect of damping on the resonance peak.
- 💡For calculation questions, ensure you use the correct formula for amplitude at resonance, such as A = F0 / (m * gamma * omega0) or A = 2Q F0 / (m omega0^2), and show all steps clearly with units.
Common Mistakes
- Saying that a forced oscillator always vibrates at its natural frequency; correct by stating that it vibrates at the driving frequency, with maximum amplitude when this equals the natural frequency.
- Confusing resonance with any large vibration; correct by linking resonance specifically to driving frequency matching natural frequency.
- Ignoring damping when describing the resonance peak; correct by explaining that damping lowers and broadens the peak.
- Thinking resonance creates energy: correct this by stating that the driver supplies the energy and resonance maximises the energy transferred per cycle.
- Confusing amplitude with frequency: correct this by keeping the axes distinct, with driving frequency on the horizontal axis and steady-state amplitude on the vertical axis.
- Assuming damping always destroys resonance: correct this by explaining that damping lowers and broadens the peak but the driven system still shows a maximum near the natural frequency.
- Treating the natural frequency as changing with damping: correct this by noting that damping mainly changes peak height and width, while the natural frequency is set by the system's inertia and stiffness.
- Describing a stationary wave as travelling along the string: correct this by stating that the wave appears to stand still because incident and reflected waves superpose.
- Ignoring boundary conditions in tubes: correct this by identifying nodes and antinodes at closed and open ends before choosing the resonant frequencies.
- Claiming damping changes the natural frequency dramatically: correct this by explaining that damping mainly reduces and broadens the resonance peak.
- Using a mechanical example without naming the driver: correct this by stating what supplies the periodic driving force, such as a motor or a vibrating support.
- Misconception: At resonance, the amplitude becomes infinite. Correction: In reality, damping always limits the amplitude to a finite maximum. Without damping, the amplitude would grow without bound, but some damping is always present.
- Misconception: The system vibrates at its natural frequency during forced vibrations. Correction: The system vibrates at the driving frequency. Only at resonance do the driving and natural frequencies coincide.
- Misconception: Resonance always leads to large amplitudes. Correction: The amplitude at resonance depends on the damping; heavy damping can significantly reduce the maximum amplitude.
Revision Plan
- 1Day 1-2: Review the basics of simple harmonic motion and damping. Ensure you can define natural frequency and understand energy transformations in oscillating systems.
- 2Day 3-4: Study forced vibrations and resonance. Learn the definitions, the conditions for resonance, and how damping affects the resonance curve. Practice sketching amplitude-frequency graphs for different damping levels.
- 3Day 5-6: Work through calculations involving resonance, such as finding maximum amplitude using quality factor or damping coefficient. Solve past paper questions on this topic.
- 4Day 7-8: Focus on applications and examples of resonance (e.g., Tacoma Narrows Bridge, microwave oven, musical instruments) and practice explaining them in terms of energy transfer.
- 5Day 9-10: Complete a full topic test under timed conditions. Review any mistakes and revisit weak areas. Use flashcards for key definitions and formulas.
Exam Question Types
- 📋Definition and explanation questions: e.g., 'Define resonance and explain why the amplitude is maximum at resonance.' Advice: Use precise terminology and refer to energy transfer and phase relationship.
- 📋Graph sketching and interpretation: e.g., 'Sketch the amplitude-frequency graph for a forced oscillator with light and heavy damping.' Advice: Label axes correctly, show resonance peak shifting and broadening with increased damping.
- 📋Calculation questions: e.g., 'Calculate the maximum amplitude of a driven oscillator at resonance given the driving force, mass, and quality factor.' Advice: Use the correct formula, show substitution, and give units.
- 📋Practical application questions: e.g., 'Explain how resonance is used in a microwave oven or why it is dangerous for bridges.' Advice: Link the phenomenon to the specific context, mentioning energy transfer and damping.
Command Word Expectations (AQA)
Give a precise, formal statement of the term. For resonance, state that it is the condition when the driving frequency equals the natural frequency, resulting in maximum amplitude. No explanation required unless asked.
Provide a reasoned account, often in terms of energy transfer or phase. For example, explain why amplitude is maximum at resonance by stating that the driving force is in phase with velocity, so maximum power is transferred.
Use the appropriate formula, substitute numerical values correctly, and give the final answer with units and appropriate significant figures. Show all working.
How Students Lose Marks (Examiner Pitfalls)
Step-by-Step Worked Solutions
Question: A mass-spring system has a natural frequency of 2.0 Hz. It is driven by an external force with a frequency of 2.0 Hz. The system has a quality factor Q of 50. Calculate the maximum amplitude of the forced oscillation if the driving force has a constant amplitude of 0.50 N and the mass is 0.20 kg. Assume the system is lightly damped.
- 1.Step 1: Identify given facts: natural frequency f0 = 2.0 Hz, driving frequency f = 2.0 Hz (resonance), Q = 50, driving force amplitude F0 = 0.50 N, mass m = 0.20 kg.
- 2.Step 2: At resonance, the amplitude A is given by A = Q * F0 / (k * m)^0.5? Actually, for a driven harmonic oscillator, the amplitude at resonance is A = F0 / (m * omega0^2 * (1/Q))? Better: Use the formula for amplitude at resonance: A = F0 / (m * gamma * omega0), where gamma = omega0 / (2Q). So A = F0 / (m * (omega0/(2Q)) * omega0) = 2Q F0 / (m omega0^2).
- 3.Step 3: Calculate angular natural frequency: omega0 = 2 * pi * f0 = 2 * pi * 2.0 = 12.566 rad/s.
- 4.Step 4: Calculate spring constant k = m * omega0^2 = 0.20 * (12.566)^2 = 0.20 * 157.91 = 31.58 N/m.
- 5.Step 5: Use formula for amplitude at resonance: A = 2Q F0 / (m omega0^2) = 2 * 50 * 0.50 / (0.20 * 157.91) = 50 / 31.58 = 1.583 m.
- 6.Step 6: State final answer with units: A = 1.6 m (2 s.f.).
Question: Explain, in terms of energy transfer, why the amplitude of a forced oscillation is maximum at resonance. (4 marks)
- 1.Step 1: At resonance, the driving frequency equals the natural frequency of the system.
- 2.Step 2: The driving force is always in phase with the velocity of the oscillator (or the phase difference between force and displacement is 90 degrees).
- 3.Step 3: This means the driving force does positive work on the oscillator at all times, transferring energy to it continuously.
- 4.Step 4: The energy transferred per cycle is maximised, leading to a large amplitude of oscillation.
- 5.Step 5: Damping removes energy, but at resonance the energy input per cycle is at its maximum, so the steady-state amplitude is highest.