PAG Flashcards

1
Q

Free fall experiment

A

Method and Calculations

  • Measure the height (h):
    • Measure the vertical distance from the bottom of the ball bearing to the trapdoor.
  • Release the ball bearing:
    • Simultaneously start the timer and disconnect the electromagnet by flicking the switch.
    • The ball bearing falls, knocking the trapdoor down, breaking the circuit, and stopping the timer.
  • Record and repeat:
    • Record the time (t) shown on the timer.
    • Repeat the experiment three times and calculate the average time.
  • Calculate acceleration due to gravity (g):
    • Use the equation: h = 0.5 * g * t2 (from page 50).
    • Rearrange to solve for g = 2h / t2.
  • Repeat for different heights:
    • Perform the experiment for several heights, calculate g for each, and average the results.

===

Analysis (y = mx + c)

  • Plot a graph:
    • Plot h (y-axis) against t2 (x-axis).
    • The graph should be linear, with the equation h = 0.5g * t2, corresponding to y = mx + c, where:
      • Gradient (m) = 0.5g.
      • y-intercept (c) = 0.
  • Determine g:
    • Calculate g = 2 * gradient.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a ruler with a high resolution to measure height (h) accurately.
    • Ensure the timer is precise and starts/stops exactly when the ball bearing is released/hits the trapdoor.
    • Repeat the experiment multiple times to reduce random errors.
  • Safety:
    • Place a cushion or soft material below the trapdoor to prevent damage or injury from the falling ball bearing.
  • Limitations:
    • Air resistance may affect the motion of the ball bearing, especially at higher heights.
    • Human reaction time may introduce errors when starting/stopping the timer manually.
    • The trapdoor mechanism may not break the circuit instantaneously.
  • Improvements:
    • Use a light gate or electronic sensor to measure time more accurately.
    • Perform the experiment in a vacuum to eliminate air resistance.
    • Use a data logger to automatically record the time and reduce human error.
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2
Q

Young’s Modulus (PAG)

A

Method and Calculations

  • Set up the wire:
    • Use a thin and long test wire for more accurate measurements, reducing uncertainty.
    • Clamp the wire to the bench and hang weights off one end, starting with the smallest weight necessary to straighten the wire.
  • Measure dimensions:
    • Find the wire’s cross-sectional area by measuring its diameter with a micrometer and using the formula for the area of a circle.
    • Measure the unstretched length from the fixed end of the wire to the marker.
  • Record extensions:
    • Record the starting position of the marker.
    • Increase the weight in steps and record the marker reading each time to determine the extension.
  • Calculate stress and strain:
    • Use the results to calculate stress and strain of the wire.
    • Plot a stress-strain curve.

===

Analysis (y = mx + c)

  • Plot a graph:
    • Plot stress (y-axis) against strain (x-axis).
    • The graph should show a linear region (Hooke’s Law) where stress ∝ strain, corresponding to y = mx + c, where:
      • Gradient (m) = Young’s modulus.
      • y-intercept (c) = 0.

===

Accuracy, Safety, Limitations, and Improvements

  • Systematic Errors:
    • Use a vernier scale for more precise readings of extension.
    • Ensure the wire returns to its original length after removing the load to avoid permanent deformation.
  • Random Errors:
    • Reduce parallax error by reading the marker carefully.
    • Repeat the experiment for all loads and calculate an average extension.
    • Measure the wire’s diameter at several points and take an average to reduce uncertainty in cross-sectional area.
  • Safety Considerations:
    • Wear safety goggles in case the wire snaps.
    • Place a cushion or soft surface below the mass hanger to catch it if it falls.
  • Improvements:
    • Use a digital micrometer for more accurate diameter measurements.
    • Ensure the wire is perfectly vertical to avoid uneven stretching.
    • Use a data logger to automatically record extensions for greater precision.
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3
Q

Resistivity (PAG)

A

Method and Calculations

  • Measure the wire dimensions:
    • Measure the diameter of the wire in at least three places and calculate the mean diameter.
    • Halve the mean diameter to find the mean radius.
    • Use the radius to calculate the cross-sectional area (A = πr²).
  • Set up the experiment:
    • Clamp the wire and attach the flying lead.
    • Close the switch and measure the current (I) and potential difference (V) across the test wire.
    • Calculate the resistance (R) using R = V/I.
  • Repeat for different lengths:
    • Reposition the flying lead for different wire lengths and repeat the process.
    • Record the mean resistance for each length.

===

Analysis (y = mx + c)

  • Plot a graph:
    • Plot average resistance (y-axis) against length (x-axis).
    • The graph should be linear, with the equation R = (ρ/A) * L, corresponding to y = mx + c, where:
      • Gradient (m) = ρ/A.
      • y-intercept (c) = 0.
  • Determine resistivity:
    • Calculate ρ = gradient × A, where A is the cross-sectional area.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a micrometer for precise diameter measurements.
    • Ensure the flying lead makes good contact to avoid inconsistent readings.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Avoid overheating by ensuring the circuit is set up correctly.
    • Handle the wire carefully to prevent injury.
  • Limitations:
    • The wire may not have a perfectly circular cross-section, affecting area calculations.
    • Temperature changes may alter the wire’s resistance.
  • Improvements:
    • Use a digital multimeter for more accurate readings.
    • Perform the experiment in a temperature-controlled environment.
    • Measure the diameter at more than three points for a better mean value.
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4
Q

Potential divider (PAG)

A

Method and Calculations

  • Set up the heat sensor:
    • Use a thermistor in a potential divider circuit (as shown in Figure 3).
    • Place the thermistor in a beaker of ice water, measure the initial temperature, and record the voltage across the thermistor.
  • Record data:
    • Gradually heat the beaker, recording the temperature and voltage at regular intervals over a suitable range.
  • Plot a graph:
    • Plot voltage (y-axis) against temperature (x-axis).

===

Analysis (y = mx + c)

  • Interpret the graph:
    • The graph should show that as temperature increases, the voltage decreases.
    • This is because the thermistor’s resistance decreases with increasing temperature, causing it to take a smaller share of the total potential difference.
    • The relationship is non-linear due to the thermistor’s exponential response to temperature.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a digital thermometer for precise temperature measurements.
    • Ensure the thermistor is fully submerged in the water for consistent readings.
    • Stir the water to maintain a uniform temperature.
  • Safety Considerations:
    • Handle the hot water carefully to avoid burns.
    • Use a heat-resistant beaker and place it on a stable surface.
  • Limitations:
    • The thermistor’s response may not be perfectly consistent due to manufacturing variations.
    • The non-linear relationship makes it harder to predict voltage changes at extreme temperatures.
  • Improvements:
    • Use a data logger to automatically record voltage and temperature for greater precision.
    • Calibrate the thermistor using known temperature points for better accuracy.
    • Repeat the experiment with a different thermistor to check for consistency.
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5
Q

Diffraction grating (PAG)

A

Method and Calculations

  • Set up the experiment:
    • Pass monochromatic light through a diffraction grating to create a pattern of bright lines (maxima) on a dark background.
    • Identify the zero-order line (central maximum) and the first-order lines on either side.
  • Measure the angle:
    • Use the small angle approximation to calculate the angle (θ) of the first-order line relative to the zero-order line, given the fringe width (x) and the distance to the screen (D).
  • Calculate the wavelength:
    • Use the formula: nλ = d sinθ, where:
      • n = order of the maximum (e.g., 1 for first-order),
      • λ = wavelength of the light,
      • d = slit separation,
      • θ = angle between the maximum and the incident light.

===

Analysis (y = mx + c)

  • Interpret the pattern:
    • The bright lines are due to constructive interference, while the dark areas result from destructive interference.
    • For white light, the pattern splits into a spectrum from red (outside) to violet (inside) for each order, with the zero-order maximum remaining white.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a laser or high-quality monochromatic light source for clear, sharp fringes.
    • Measure the distance to the screen (D) and fringe width (x) carefully to minimize errors in calculating θ.
  • Safety Considerations:
    • Avoid looking directly into the laser beam or bright light sources to protect your eyes.
    • Ensure the setup is stable to prevent the diffraction grating or screen from moving during the experiment.
  • Limitations:
    • The small angle approximation may introduce errors for larger angles.
    • The diffraction grating may have imperfections, leading to less distinct fringes.
  • Improvements:
    • Use a vernier scale or digital caliper to measure fringe widths more accurately.
    • Repeat the experiment with different slit separations (d) to verify consistency.
    • Use a spectrometer for more precise angle measurements.
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6
Q

Plank constant (PAG)

A

Method and Calculations

  • Set up the experiment:
    • Use monochromatic LEDs emitting a single wavelength of light.
    • Set the variable resistor to its maximum resistance to prevent current flow initially.
  • Measure threshold voltage (V₀):
    • In a dark room, adjust the resistor until the LED just begins to light up.
    • Record the threshold voltage (V₀) and the wavelength (λ) of the emitted light.
  • Repeat and average:
    • Repeat the experiment multiple times, averaging the results for V₀.
    • Perform the experiment for a range of LEDs with different wavelengths.
  • Plot a graph:
    • Plot threshold voltage (V₀) against the inverse of the wavelength (1/λ).
    • The graph should be a straight line with the gradient = hc/e.
  • Calculate Planck constant (h):
    • Use the gradient to calculate h = (gradient × e) / c.

===

Analysis (y = mx + c)

  • Interpret the graph:
    • The equation eV₀ = hc/λ corresponds to y = mx + c, where:
      • y = V₀,
      • x = 1/λ,
      • gradient (m) = hc/e,
      • y-intercept (c) = 0.
  • Determine Planck constant (h):
    • Substitute the gradient into the equation h = (gradient × e) / c.

Accuracy, Safety, Limitations, and Improvements

  • Systematic Errors:
    • Human error in identifying the exact voltage at which the LED begins to glow.
    • Use a black viewing tube in a darkened room for better accuracy.
    • A more accurate method: Plot a current vs. voltage graph and extrapolate to find the threshold voltage.
  • Random Errors:
    • LEDs emit a narrow spectrum of light (∼60 nm width), not a single frequency.
    • The quoted wavelength is the central wavelength, but the lower end is emitted when the LED just glows, introducing error.
  • Safety Considerations:
    • Do not stare directly at brightly lit LEDs, especially blue LEDs (close to UV).
    • Limit current to ≤ 50 mA (check LED ratings) to avoid damage.
    • Use a 330 Ω resistor to limit current.
    • Potentiometer hazard: Incorrect wiring can cause short circuits, leading to overheating and fire.
      • Turn off power immediately if burning is smelled.
    • Keep water away from electrical equipment.
  • Improvements:
    • Use a spectrometer to measure the exact wavelength of light emitted by the LED.
    • Use a data logger to record voltage and current more accurately.
    • Repeat the experiment with a wider range of LEDs to improve the reliability of the graph.
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7
Q

Internal resistance (PAG)

A

Method and Calculations

  • Set up the circuit:
    • Set the variable resistor to its highest resistance.
    • Record the current (I) and potential difference (V) across the circuit.
  • Repeat measurements:
    • Adjust the load resistance and repeat the measurements for multiple values.
    • Calculate the mean current and voltage for each resistance.
  • Plot a graph:
    • Plot a V-I graph with mean data points and draw a line of best fit.
    • Ensure all variables, including temperature, are kept constant.
  • Analyze results:
    • Determine the gradient (-r) and intercept (E) from the graph.
    • Use the equation V = E - Ir, where:
      • E = electromotive force (e.m.f.),
      • r = internal resistance.

===

Analysis (y = mx + c)

  • Interpret the graph:
    • The equation V = E - Ir corresponds to y = mx + c, where:
      • y = V,
      • x = I,
      • gradient (m) = -r,
      • y-intercept (c) = E.
  • Determine internal resistance and e.m.f.:
    • The gradient gives the internal resistance (r).
    • The y-intercept gives the e.m.f. (E).

===

Accuracy, Safety, Limitations, and Improvements

  • Systematic Errors:
    • Close the switch briefly to take readings, preventing changes in the internal resistance of the battery.
  • Random Errors:
    • Use fairly new cells to avoid variations in e.m.f. and internal resistance.
    • Wait for readings to stabilise before recording.
    • Take multiple repeats (at least 3) and calculate a mean to reduce errors.
  • Safety Considerations:
    • Electrical components can get hot with prolonged use.
    • Switch off the power supply if burning is smelled.
    • Keep liquids away from equipment to avoid damage.
  • Improvements:
    • Use a data logger to record current and voltage automatically for greater precision.
    • Perform the experiment in a temperature-controlled environment to minimize thermal effects.
    • Use a digital multimeter for more accurate measurements of current and voltage.
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8
Q

Oscilloscope (PAG)

A

Cathode Ray Oscilloscope (CRO):

  • Displays voltage over time from a signal generator, known as a trace.
  • The type of trace depends on the source:
    • AC supply: Produces a trace that alternates between positive and negative patterns.
    • Sound waves: Converted into electrical signals by a microphone can also be displayed.

===

Oscilloscope Screen:

  • Divided into divisions:
    • Vertical axis: Represents volts.
    • Horizontal axis: Represents time.
  • Volts per division and seconds per division are controlled by the gain and timebase dials, respectively.

===

Wave Properties:

  • Oscilloscope traces can be used to calculate:
    • Frequency: 1 ÷ period
    • Period: Measured using the timebase.
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9
Q

Polarising filters for light (PAG)

A

Polarisation:

  • Observed by shining unpolarised light through two polarising filters aligned vertically and rotating the second filter.
  • Rotating the second filter reduces light intensity as its transmission axis deviates from vertical.

===

Key Observations:

  • At 45 degrees between transmission axes:
    • Intensity through the second filter is half that of the first.
  • At right angles (90 degrees):
    • No light passes through.
  • After 180-degree rotation:
    • Transmission axes realign, allowing all light through.

===

Applications:

  • Polaroid sunglasses: Use polarising filters to block partially polarised light, reducing glare.
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10
Q

Speed of sound (PAG)

A

Method and Calculations

  • Set up the experiment:
    • Place a hollow tube in water to create a closed-end pipe.
    • Note the frequency (f) of a tuning fork and hold it above the tube.
  • Produce resonance:
    • Tap the tuning fork gently to produce sound waves that travel down the tube and reflect at the air/water surface.
    • Adjust the tube’s height until the sound resonates the loudest, indicating the lowest resonant frequency of the closed tube.
  • Measure and calculate:
    • The tube’s length at resonance is a quarter of the sound wave’s wavelength (λ/4).
    • Use the frequency and wavelength to calculate the speed of sound in air using the equation:
      • v = fλ.

===

Analysis

  • Resonance condition:
    • For a closed pipe, the lowest resonant frequency occurs when the tube length is λ/4.
    • The relationship between the tube length (L) and wavelength (λ) is: L = λ/4.
  • Calculate speed of sound:
    • Rearrange the equation to find λ = 4L.
    • Substitute λ and the known frequency (f) into v = fλ to calculate the speed of sound.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the tuning fork is struck gently to avoid overtones that could distort the resonance.
    • Measure the tube length carefully using a ruler with high precision.
    • Repeat the experiment to confirm the resonant length and calculate an average value.
  • Safety Considerations:
    • Handle the tuning fork carefully to avoid injury or damage.
    • Ensure the tube is stable to prevent spills or accidents.
  • Limitations:
    • The air/water surface may not be perfectly flat, affecting the reflection of sound waves.
    • Background noise can make it difficult to detect the loudest resonance.
  • Improvements:
    • Use a microphone and oscilloscope to detect resonance more accurately.
    • Perform the experiment in a quiet environment to minimize interference.
    • Repeat with tuning forks of different frequencies to verify consistency.
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11
Q

Semi circle light rays (PAG)

A

Method and Calculations

  • Set up the experiment:
    • Place the glass block on paper and shine light from the ray box into the curved surface of the block.
  • Find the critical angle:
    • Rotate either the ray box or the glass block until the refracted ray from the glass block makes an angle of 90° (grazes the surface).
    • Use a protractor to measure the angle of incidence (c) of the ray of light within the block; this is the critical angle.
  • Calculate refractive index:
    • Use the formula: n = (sin c)–1 to calculate the refractive index (n) of the glass block.

===

Analysis

  • Critical angle and refraction:
    • At the critical angle (c), the refracted ray travels along the boundary between the glass and air (angle of refraction = 90°).
    • The relationship between the refractive index (n) and the critical angle (c) is given by:
      • n = 1 / sin c.
  • Interpretation:
    • A higher refractive index corresponds to a smaller critical angle, indicating greater bending of light.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the ray box produces a narrow, well-defined beam of light for precise measurements.
    • Use a protractor with high precision to measure the angle of incidence.
    • Repeat the experiment to confirm the critical angle and calculate an average value.
  • Safety Considerations:
    • Handle the glass block carefully to avoid breakage or injury.
    • Avoid shining the light directly into eyes.
  • Limitations:
    • The curved surface of the glass block may introduce errors in measuring the angle of incidence.
    • The ray box may produce a beam that is not perfectly collimated, affecting accuracy.
  • Improvements:
    • Use a semicircular glass block to simplify the alignment of the incident and refracted rays.
    • Perform the experiment in a darkened room to improve visibility of the light beam.
    • Use a digital angle finder for more precise angle measurements.
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12
Q

Center of mass (PAG)

A
  1. Hang an object from a single point; the centre of mass will lie directly below that point.
  2. Hang the object from two different points and draw a plumb line (a vertical line) from each point.
  3. The intersection of these two lines is the centre of mass.
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13
Q

Specific Heat Capacity (PAG)

A

Measuring Specific Heat Capacity

  • Measure initial conditions:
    • Measure the mass (m) and initial temperature (T₁) of the substance.
  • Heat the substance:
    • Use a heater to heat the substance, monitoring the change in temperature (ΔT).
    • Measure the current (I) and voltage (V) across the heater, and record the time (t) it is on.
  • Calculate energy supplied:
    • Use the formula: E = V × I × t.
  • Calculate specific heat capacity (c):
    • Use the formula: E = m × c × ΔT.
    • Rearrange to find: c = E / (m × ΔT).

Estimating Specific Heat Capacity Using Mixing Method

  • Mix hot and cold substances:
    • Mix a hot substance (mass m₁, specific heat capacity c₁, initial temperature T₁) with a cold substance (mass m₂, specific heat capacity c₂, initial temperature T₂).
    • Measure the final temperature (T₀) once thermal equilibrium is reached.
  • Calculate specific heat capacity:
    • Use the formula: m₁c₁(T₁ - T₀) = m₂c₂(T₀ - T₂).
    • Rearrange to find the unknown specific heat capacity (c₁ or c₂).

===

Analysis

  • Energy transfer:
    • In the heating method, the energy supplied by the heater is equal to the energy absorbed by the substance.
    • In the mixing method, the energy lost by the hot substance is equal to the energy gained by the cold substance (assuming no heat loss to the surroundings).
  • Assumptions:
    • No heat is lost to the surroundings in the mixing method.
    • The heater is 100% efficient in the heating method.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a thermometer with high precision to measure temperature changes.
    • Ensure the heater is fully submerged and the substance is well-insulated to minimize heat loss.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Handle hot substances carefully to avoid burns.
    • Ensure electrical equipment (e.g., heater) is properly insulated to prevent electric shocks.
  • Limitations:
    • Heat loss to the surroundings can affect results in both methods.
    • The mixing method assumes no heat loss, which is not always realistic.
  • Improvements:
    • Use a calorimeter to minimize heat loss in the mixing method.
    • Perform the experiment in a temperature-controlled environment.
    • Use a data logger to monitor temperature changes continuously.
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14
Q

Specific Latent Heat (PAG)

A

Method and Calculations

Measuring Specific Latent Heat of Fusion

  • Set up the experiment:
    • Use a heating coil in one funnel of ice.
    • Connect the coil to an ammeter and voltmeter.
  • Heat the ice:
    • Turn the heater on for three minutes and measure the current (I) and voltage (V).
    • Calculate the energy transferred using W = VIt.
  • Measure melted ice:
    • Use a second unheated funnel to measure the mass of ice melted at room temperature.
    • Subtract the unheated mass from the heated mass to find the mass of ice melted due to the heater (m).
  • Calculate latent heat of fusion:
    • Use the formula: E = mL, where L is the specific latent heat of fusion.
    • Rearrange to find: L = E/m.

Measuring Specific Latent Heat of Vaporisation

  • Set up the experiment:
    • Place a heating coil in a beaker of water, and insulate the outside of the beaker.
    • Connect the coil to an ammeter and voltmeter.
  • Heat the water:
    • Start heating the water and monitor the mass of water as it boils, using a mass balance.
    • Measure the voltage (V) and current (I) across the heating coil.
    • Once the mass decreases by about 15 g, stop the timer.
  • Calculate energy transferred:
    • Use the formula: W = VIt.
  • Calculate latent heat of vaporisation:
    • Use the formula: L = E/m, where E is the energy transferred and m is the mass lost.

===

Analysis

  • Energy transfer:
    • In both experiments, the energy supplied by the heater is used to change the state of the substance (ice to water or water to steam) without changing its temperature.
  • Key equations:
    • For fusion: E = mLf.
    • For vaporisation: E = mLv.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a high-precision mass balance to measure the mass of ice or water.
    • Ensure the heating coil is fully submerged and the system is well-insulated to minimize heat loss.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Handle hot water and steam carefully to avoid burns.
    • Ensure electrical equipment (e.g., heater) is properly insulated to prevent electric shocks.
  • Limitations:
    • Heat loss to the surroundings can affect results.
    • The mass of ice melted at room temperature may vary due to environmental factors.
  • Improvements:
    • Use a calorimeter to minimize heat loss.
    • Perform the experiment in a temperature-controlled environment.
    • Use a data logger to monitor temperature and mass changes continuously.
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15
Q

Boyle’s Law (PAG)

A

Method and Calculations

  • Set up the apparatus:
    • Use a sealed tube containing air and oil, a Bourdon gauge for pressure measurement, and a tyre pump to vary pressure.
  • Measure pressure and volume:
    • Increase pressure by pumping air into the system.
    • Measure pressure (p) with the Bourdon gauge.
    • Calculate volume (V) by multiplying the length of the air-containing part of the tube by the tube’s cross-sectional area (A = πr²).
  • Record data:
    • Gradually increase pressure at set intervals and wait for temperature to stabilize before recording readings.
    • Multiply pressure and volume at each point; they should give the same value if Boyle’s Law is valid.
  • Repeat and average:
    • Repeat the experiment and calculate the mean for each reading.

===

Analysis

  • Boyle’s Law verification:
    • Boyle’s Law states that pV = constant for a fixed mass of gas at constant temperature.
    • The product of pressure (p) and volume (V) should remain constant if the law holds.
  • Graph plotting:
    • Plot pressure (p) against volume (V).
    • The graph should show a hyperbolic curve, confirming the inverse proportionality between pressure and volume.
    • Alternatively, plot p against 1/V to obtain a straight line passing through the origin.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the temperature remains constant throughout the experiment.
    • Use a high-precision Bourdon gauge for accurate pressure measurements.
    • Measure the length of the air column carefully using a ruler with high resolution.
  • Safety Considerations:
    • Avoid over-pressurising the system to prevent the tube or gauge from bursting.
    • Handle the tyre pump carefully to avoid injury.
  • Limitations:
    • The oil in the tube may introduce errors if it affects the air volume or pressure measurements.
    • The assumption of constant temperature may not hold if the experiment is conducted too quickly.
  • Improvements:
    • Use a digital pressure sensor for more accurate and consistent readings.
    • Perform the experiment in a temperature-controlled environment.
    • Repeat the experiment multiple times to reduce random errors.
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16
Q

Absolute Zero (PAG)

A

Method and Calculations

  • Set up the apparatus:
    • Submerge a stoppered flask filled with air into a beaker of water.
    • Connect the stopper to a Bourdon gauge with tubing (ensure the tubing’s volume is much smaller than the flask’s volume).
  • Record initial conditions:
    • Record the temperature of the water and the pressure on the Bourdon gauge.
  • Heat the water:
    • Insert an electric heater, heat the water for a few minutes, then remove it.
    • Stir the water to ensure a uniform temperature and allow time for heat transfer to the air inside the flask.
    • Record the pressure and temperature.
  • Repeat and average:
    • Repeat several times, heating the water incrementally until it starts to boil.
    • Repeat the entire experiment twice more with fresh cool water.

===

Analysis

  • Pressure Law verification:
    • The Pressure Law states that p/T = constant for a fixed mass of gas at constant volume.
    • Multiplying pressure (p) and temperature (T) together should yield a constant if the law holds.
  • Graph plotting:
    • Plot pressure (p) against temperature (T).
    • Draw a line of best fit and extrapolate it to the x-axis to estimate the value of absolute zero.
    • The graph should be a straight line passing through the origin when temperature is in Kelvin.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the temperature is uniform by stirring the water thoroughly.
    • Use a high-precision thermometer and Bourdon gauge for accurate measurements.
    • Repeat the experiment multiple times to reduce random errors.
  • Safety Considerations:
    • Handle the electric heater carefully to avoid burns or electric shocks.
    • Avoid overheating the water to prevent the flask or tubing from cracking.
  • Limitations:
    • The Bourdon gauge may have a limited range, affecting measurements at high pressures.
    • Heat loss to the surroundings may affect the accuracy of temperature measurements.
  • Improvements:
    • Use a digital pressure sensor and temperature probe for more accurate and consistent readings.
    • Perform the experiment in a temperature-controlled environment.
    • Insulate the beaker to minimize heat loss to the surroundings.
17
Q

Circular Motion (PAG)

A

Method and Calculations

  • Set up the apparatus:
    • Attach a bung to a string threaded through a plastic tube.
    • Weigh the washers used to anchor the free end of the string.
    • Measure the radius (r), which is the distance from the bung to the reference mark.
  • Spin the bung:
    • Rotate the bung in a horizontal circle while keeping the reference mark level with the tube’s top.
    • Adjust the speed to prevent the mark from moving.
  • Measure time period:
    • Record the time (T) for one complete circle or multiple circles for greater accuracy.
  • Calculate angular speed:
    • Use the formula: ⍵ = 2π/T.
  • Calculate centripetal force:
    • Use the formula: F = m⍵²r, where m is the mass of the bung.

===

Analysis

  • Observation:
    • Repeat the experiment for different values of r.
    • As r increases, the time period (T) lengthens, but the centripetal force remains constant, equal to the weight of the washers (W = mg).
  • Key relationships:
    • The centripetal force is provided by the tension in the string, which is balanced by the weight of the washers.
    • The relationship between radius (r), angular speed (⍵), and centripetal force (F) is given by F = m⍵²r.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the reference mark remains level with the tube’s top to maintain a constant radius.
    • Use a stopwatch to measure the time period accurately.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Ensure the string is securely attached to the bung and tube to prevent it from slipping or breaking.
    • Spin the bung carefully to avoid hitting nearby objects or people.
  • Limitations:
    • Air resistance may affect the motion of the bung, especially at high speeds.
    • The string may stretch slightly, introducing errors in the measurement of r.
  • Improvements:
    • Use a light gate or motion sensor to measure the time period more accurately.
    • Perform the experiment in a controlled environment to minimize air resistance.
    • Use a stiffer string to reduce stretching.
18
Q

SHM (PAG)

A

Method and Calculations

Using Sensors and a Data Logger

  • Set up the experiment:
    • Use a position sensor connected to a data logger to record the displacement-time graph for a mass-spring system oscillating in SHM.
  • Analyze the graph:
    • Measure the amplitude (A) and time period (T) from the graph.
    • Calculate the frequency (f) using f = 1/T.
  • Observe energy loss:
    • As oscillations progress, the amplitude decreases due to energy loss, but the time period and frequency remain constant.

Without Sensors and a Data Logger

  • Set up the pendulum:
    • Use a pendulum setup with a ruler, protractor, and stopwatch.
    • Measure the length of the string, mass weight, and initial displacement angle (<10°) for accurate results.
  • Record oscillations:
    • Record the time period (T) for several oscillations and calculate the frequency (f) using f = 1/T.
  • Investigate variables:
    • Changing the string length affects T, but mass and angle have no effect on T.

===

Analysis

  • SHM characteristics:
    • In SHM, the time period (T) and frequency (f) are independent of amplitude and mass (for a pendulum).
    • The displacement-time graph for SHM is sinusoidal, showing the relationship between displacement and time.
  • Energy loss:
    • In real systems, energy is lost due to air resistance or friction, causing the amplitude to decrease over time.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • For the mass-spring system, ensure the position sensor is calibrated correctly.
    • For the pendulum, measure the string length and angle carefully using a ruler and protractor.
    • Use a stopwatch with high precision to measure time periods.
  • Safety Considerations:
    • Ensure the pendulum setup is stable to prevent the mass from swinging into nearby objects or people.
    • Handle the mass-spring system carefully to avoid injury from the spring or mass.
  • Limitations:
    • Air resistance and friction can affect the accuracy of results, especially in the mass-spring system.
    • Manual measurements (e.g., stopwatch) may introduce human error.
  • Improvements:
    • Use a light gate or motion sensor to measure time periods more accurately for the pendulum.
    • Perform the experiment in a vacuum or controlled environment to minimize air resistance.
    • Repeat measurements multiple times to reduce random errors.
19
Q

Capacitors in Series and Parallel (PAG)

A

Method and Calculations

Capacitors in Series

  • Set up the circuit:
    • Connect three identical capacitors in series.
    • Set the variable resistor to a high resistance value and record it.
  • Charge the capacitors:
    • Close the switch to start charging the capacitors.
    • Record the initial current in the circuit.
    • Use a data logger connected to a voltmeter to record the potential difference across the capacitors over time.
    • Adjust the variable resistor to maintain a constant current as much as possible.
  • Monitor the current:
    • Once the capacitors are fully charged (current drops to zero), open the switch.

Capacitors in Parallel

  • Set up the circuit:
    • Connect another three identical capacitors in parallel.
    • Repeat the same steps as for the series circuit, ensuring the variable resistor starts at the same resistance value.

===

Analysis

  • Plot a charge vs. potential difference graph for each circuit, using ΔQ = IΔt to calculate the charge stored by the capacitors at each time reading.
  • Graph interpretation:
    • The charge vs. potential difference graph should be a straight line through the origin, with the gradient representing the total capacitance of the circuit.
  • Compare results:
    • Compare the experimental total capacitance (from the gradient) with the theoretical values for capacitors in series and parallel:
      • Series: 1/Ctotal = 1/C1 + 1/C2 + 1/C3.
      • Parallel: Ctotal = C1 + C2 + C3.
  • Accuracy:
    • Use a high-precision voltmeter and ammeter for accurate measurements.
    • Ensure the variable resistor is adjusted smoothly to maintain a constant current.
    • Repeat the experiment to reduce random errors.
  • Safety Considerations:
    • Handle the capacitors carefully to avoid short circuits or electric shocks.
    • Ensure the circuit is properly insulated and connections are secure.
  • Limitations:
    • Maintaining a constant current may be difficult as the capacitors approach full charge.
    • The capacitors may have slight variations in capacitance, affecting results.
  • Improvements:
    • Use a digital data logger for more precise and automated recordings.
    • Perform the experiment in a controlled environment to minimize external interference.
    • Use capacitors with known and identical capacitance values for better comparison.
20
Q

Investigating Charging and Discharging Capacitors (PAG)

A

Method and Calculations

Investigating Charging a Capacitor

  • Set up the circuit:
    • Use a fixed resistor to slow down the charging process.
    • Connect a voltmeter and ammeter to measure potential difference and current, respectively.
  • Charge the capacitor:
    • Close the switch to begin charging the capacitor.
    • Use a data logger to record potential difference and current over time.
    • Observe the current: When it drops to zero, the capacitor is fully charged.
  • Plot graphs:
    • Plot current, potential difference, and charge (ΔQ = IΔt) against time.

Investigating Discharging a Capacitor

  • Discharge the capacitor:
    • Open the switch and disconnect the power supply.
    • Close the switch to allow the capacitor to discharge.
    • Use the data logger to record potential difference and current over time.
    • Observe the current: When it reaches zero, the capacitor is fully discharged.
  • Plot graphs:
    • Plot current, potential difference, and charge (ΔQ = IΔt) against time.

===

Analysis

Charging a Capacitor

  • Initial conditions:
    • At the start, the current is high because the potential difference across the capacitor is zero.
  • During charging:
    • As the capacitor charges, the potential difference across it increases, causing the current to decrease.
    • The charge (Q) on the capacitor is directly proportional to the potential difference (V) across it (Q = CV).

Discharging a Capacitor

  • Initial conditions:
    • At the start of discharging, the current is high.
  • During discharging:
    • As charge leaves the plates, the potential difference decreases, and the current reduces.
    • The charge (Q) and potential difference (V) decrease exponentially over time.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a high-precision voltmeter and ammeter for accurate measurements.
    • Ensure the data logger records data at regular intervals for consistent results.
    • Repeat the experiment to reduce random errors.
  • Safety Considerations:
    • Handle the capacitor carefully to avoid electric shocks, especially when fully charged.
    • Ensure the circuit is properly insulated and connections are secure.
  • Limitations:
    • The fixed resistor may heat up during the experiment, affecting its resistance.
    • The capacitor may have a slight leakage current, affecting discharge measurements.
  • Improvements:
    • Use a digital data logger for more precise and automated recordings.
    • Perform the experiment in a controlled environment to minimize external interference.
    • Use capacitors with low leakage for more accurate results.
21
Q

Magnetic Flux Density (PAG)

A

Method and Calculations

  • Set up the experiment:
    • Position a square hoop of metal wire so that the top of the hoop (length L) is perpendicular to the magnetic field.
    • Connect the d.c. power supply to a variable resistor to control the current.
    • Place the setup on a digital balance and zero it when there is no current.
  • Measure force and current:
    • Turn on the d.c. power supply and ensure the mass reading is positive (if negative, swap the crocodile clips).
    • Record the mass and current for different values of current using the variable resistor.
    • Repeat for a large range of currents, taking three readings for each current to improve accuracy.
  • Convert mass to force:
    • Use F = mg to convert mass readings to force.
  • Plot a graph:
    • Plot force (F) against current (I) and draw a line of best fit.

===

Analysis

  • Graph interpretation:
    • The graph should pass through the origin, showing that force is proportional to current.
    • The gradient of the line is equal to B / L, where:
      • B = magnetic flux density,
      • L = length of the wire in the magnetic field.
  • Calculate magnetic flux density (B):
    • Use the formula: B = gradient × L.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the wire length (L) is measured accurately using a ruler with high precision.
    • Use a high-precision digital balance to measure mass.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Handle the d.c. power supply carefully to avoid short circuits or electric shocks.
    • Ensure the setup is stable to prevent the wire or balance from moving during the experiment.
  • Limitations:
    • The magnetic field may not be perfectly uniform, affecting results.
    • The wire may heat up due to high currents, altering its resistance and affecting measurements.
  • Improvements:
    • Use a stronger and more uniform magnetic field for more consistent results.
    • Perform the experiment in a temperature-controlled environment to minimize thermal effects.
    • Use a data logger to automate current and force measurements for greater precision.
22
Q

Magnetic Flux (PAG)

A

Method and Calculations

  1. Set up the magnets:
    • Place two bar magnets a small distance apart with opposite poles facing each other.
    • Ensure they are far enough apart not to snap together but close enough to create a uniform magnetic field.
  2. Prepare the search coil:
    • Use a search coil with a known number of turns (N) and area (A).
    • Connect the coil to a data recorder set to measure the induced e.m.f. with a very small time interval between readings.
  3. Position the coil:
    • Place the search coil in the middle of the magnetic field, ensuring the coil’s area is parallel to the surface of the magnets.
    • Start the data recorder.
  4. Induce e.m.f.:
    • While keeping the coil in the same orientation, move the coil out of the magnetic field immediately.
    • As the coil moves out, the e.m.f. is induced due to the changing magnetic flux linkage, going from maximum (NΦ) to zero.
  5. Plot and calculate:
    • Use the data from the recorder to plot a graph of induced e.m.f. against time.
    • Estimate the area under the graph to calculate the change in flux linkage using Faraday’s Law.
    • The change in flux linkage equals the flux linkage in the uniform magnetic field (since the final flux linkage is zero).
    • Calculate Φ using: Φ = (change in flux linkage) / N.
  6. Repeat:
    • Repeat the experiment multiple times and calculate the mean value of Φ to improve precision.

===

Analysis

  • Faraday’s Law:
    • The induced e.m.f. is proportional to the rate of change of magnetic flux linkage.
    • The area under the e.m.f. vs. time graph represents the change in flux linkage.
  • Flux linkage calculation:
    • Flux linkage (NΦ) is the product of the number of turns (N) and the magnetic flux (Φ).
    • Use Φ = (change in flux linkage) / N to find the magnetic flux in the uniform field.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Ensure the search coil is moved out of the magnetic field quickly and smoothly to avoid inconsistent readings.
    • Use a high-precision data recorder to measure the induced e.m.f. accurately.
    • Repeat the experiment multiple times to reduce random errors.
  • Safety Considerations:
    • Handle the magnets carefully to avoid pinching or injury.
    • Ensure the setup is stable to prevent the magnets or coil from moving unexpectedly.
  • Limitations:
    • The magnetic field may not be perfectly uniform, affecting results.
    • The search coil may have slight variations in its area or number of turns.
  • Improvements:
    • Use a stronger and more uniform magnetic field for more consistent results.
    • Perform the experiment in a controlled environment to minimize external interference.
    • Use a calibrated search coil with precise dimensions and turns.
23
Q

Transformers (PAG)

A

Method and Calculations

Relationship Between Turns and Voltage

  • Set up the transformer:
    • Use two cores with wire wrapped around them to form primary and secondary coils.
    • Start with a turns ratio of 1:2 (e.g., 5 turns in the primary coil and 10 in the secondary coil).
  • Measure voltages:
    • Turn on the a.c. supply at a low voltage for safety.
    • Measure the voltage across each coil while keeping the primary voltage constant.
  • Repeat for other ratios:
    • Repeat the experiment for other turns ratios, such as 1:1 and 2:1.
  • Calculate ratios:
    • Calculate n₁/n₂ (turns ratio) and V₁/V₂ (voltage ratio).
    • The ratios should be equal, confirming V₁/V₂ = n₁/n₂.

Relationship Between Current and Voltage

  • Modify the setup:
    • Add a variable resistor and ammeters to the transformer setup.
  • Record current and voltage:
    • Record the current (I₁) and voltage (V₁) across the primary coil, and current (I₂) and voltage (V₂) across the secondary coil.
    • Adjust the variable resistor to change the input current, recording the corresponding values for both coils.
  • Confirm power conservation:
    • For each current, confirm P = V₁I₁ = V₂I₂ (power remains constant, neglecting losses).

===

Analysis

  • Turns and voltage relationship:
    • The voltage ratio (V₁/V₂) is equal to the turns ratio (n₁/n₂), confirming the transformer equation: V₁/V₂ = n₁/n₂.
  • Current and voltage relationship:
    • The power in the primary coil (V₁I₁) should equal the power in the secondary coil (V₂I₂), assuming no energy losses.
    • This confirms the principle of energy conservation in an ideal transformer.

===

Accuracy, Safety, Limitations, and Improvements

  • Accuracy:
    • Use a high-precision voltmeter and ammeter for accurate measurements.
    • Ensure the a.c. supply is stable and set to a low voltage for safety and consistency.
    • Repeat measurements to reduce random errors.
  • Safety Considerations:
    • Handle the a.c. supply carefully to avoid electric shocks.
    • Ensure the setup is properly insulated and connections are secure.
  • Limitations:
    • Real transformers have energy losses (e.g., heat, eddy currents), which may cause slight deviations from ideal results.
    • The magnetic field may not be perfectly uniform, affecting the transformer’s efficiency.
  • Improvements:
    • Use a digital data logger to automate voltage and current measurements for greater precision.
    • Perform the experiment in a controlled environment to minimize external interference.
    • Use laminated cores to reduce eddy current losses.
24
Q

Terminal Velocity in Fluids

A

Method and Calculations

  • Set up the experiment:
    • Wrap elastic bands or mark intervals on a tube of viscous liquid using a ruler.
    • Release a ball bearing from rest above the liquid.
  • Record data:
    • Use a stopwatch to record the time it takes for the ball bearing to reach each mark.
    • Calculate the average speed between intervals using speed = distance / time.
  • Repeat and average:
    • Repeat the experiment multiple times for a range of readings to improve accuracy.

===

Analysis

  • Terminal velocity:
    • When the ball bearing reaches terminal velocity, the distance between intervals becomes constant.
  • Plot a velocity-time graph:
    • The graph should show the velocity increasing initially and then plateauing (zero gradient) at terminal velocity.

===

Accuracy, Safety, Limitations, and Improvements

Systematic Errors:
- Use a more viscous or denser fluid to slow the ball bearing and make terminal velocity easier to observe.
- Use a taller tube to allow the ball bearing to travel longer at terminal velocity.
- Use larger intervals to reduce percentage uncertainty in distance and time measurements.

Random Errors:
- Repeat the experiment at least four times to reduce random errors.
- Use ticker tape or a motion sensor instead of a stopwatch for more precise time measurements.

Safety Considerations:
- Handle the viscous liquid carefully to avoid spills or contamination.
- Ensure the tube is stable and securely placed to prevent accidents.

Limitations:
- The viscosity of the liquid may change with temperature, affecting results.
- Human reaction time may introduce errors when using a stopwatch.

Improvements:
- Use a digital motion sensor to track the ball bearing’s position and velocity automatically.
- Perform the experiment in a temperature-controlled environment to minimize changes in viscosity.
- Use a larger ball bearing to reduce the effect of random fluctuations in motion.

25
Q

Ripple Tank (PAG)

A

Apparatus Setup:

  • Motorized bar produces plane waves (straight wavefronts)
  • Small dipper produces circular waves
  • Overhead light source projects wave patterns onto screen below
  • Glass sheet (for refraction experiments)
  • Barriers (for reflection/diffraction studies)

===

Key Wave Properties Demonstrated:

  1. Wave Visualization:
    • Bright bands on screen represent wave crests
    • Enables direct measurement of wavelength (λ)
    • Clear observation of wavefronts and their behavior
  2. Wave Phenomena:
    • Reflection:
      • Use plane/curved surfaces
      • Measure angles of incidence/reflection relative to normal
      • Verify law of reflection (θi = θr)
    • Refraction:
      • Glass sheet creates shallow region (changes wave speed)
      • Observe wavelength change at boundary
      • Wavefronts closer together = slower speed (and vice versa)
    • Diffraction:
      • Observe wave bending around barriers
      • Most noticeable when gap width ≈ wavelength
    • Interference:
      • Two dippers produce overlapping circular waves
      • Observe constructive/destructive interference patterns

===

Experimental Control:
- Adjust motor frequency to change wavelength
- Vary bar angle to change wave direction
- Modify water depth to alter wave speed

===

Practical Considerations:
- Ensure water depth is uniform for baseline measurements
- Use stroboscopic lighting to ‘freeze’ wave patterns
- Calibrate measurements using known barrier spacing

===

Key Relationships Demonstrated:
- v = fλ (wave equation)
- n = c/v (refractive index)
- sinθi/sinθr = n (Snell’s Law)

26
Q

Alpha, Beta & Gamma Radiation (PAG)

A

Safety Protocols

  • Storage: Keep radioactive sources in a lead-lined box when not in use
  • Handling: Use long-handled tongs (minimum 30cm length)
  • Positioning:
    • Maintain >50cm distance from active sources
    • Never point sources toward people
  • PPE: Wear lab coat, gloves, and safety goggles

===

Equipment Setup

  1. Geiger-Müller tube connected to counter
  2. Radioactive sources (α, β, γ) - clearly labeled
  3. Test materials (paper, aluminum, lead sheets of varying thicknesses)
  4. Measuring ruler for precise source-detector distances

===

Experimental Procedure

A. Baseline Measurements
1. Measure background radiation:
- 3 x 30-second readings (no source present)
- Calculate mean background count rate (counts/sec)

  1. Measure source radiation:
    • Position source 5cm from GM tube
    • Take 3 x 30-second readings
    • Calculate net count rate (source rate - background)

B. Penetration Tests
1. Material Testing:
- Insert test material between source and detector
- Record count rate changes for:
- Paper (α test)
- 2mm aluminum (β test)
- 5mm lead (γ test)

  1. Quantitative Analysis:
    • For γ radiation:
      • Measure count rate through lead sheets (0.5mm to 10mm thickness)
      • Plot absorption curve (count rate vs thickness)

C. Distance Investigation
1. Vary source-detector distance (5-50cm)
2. Verify inverse square law for γ radiation

===

Data Analysis

  • Absorption Calculation:
    % absorption = 100 × (1 - (net count with material/net count without))
  • Half-Value Thickness:
    Determine thickness required to halve radiation intensity

===

Common Experimental Errors

  1. Not accounting for dead time in GM tube at high count rates
  2. Inconsistent source-detector alignment
  3. Neglecting to subtract background from all measurements