PAG Flashcards
Free fall experiment
Method and Calculations
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Measure the height (h):
- Measure the vertical distance from the bottom of the ball bearing to the trapdoor.
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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.
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Record and repeat:
- Record the time (t) shown on the timer.
- Repeat the experiment three times and calculate the average time.
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Calculate acceleration due to gravity (g):
- Use the equation: h = 0.5 * g * t2 (from page 50).
- Rearrange to solve for g = 2h / t2.
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Repeat for different heights:
- Perform the experiment for several heights, calculate g for each, and average the results.
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Analysis (y = mx + c)
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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.
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Determine g:
- Calculate g = 2 * gradient.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety:
- Place a cushion or soft material below the trapdoor to prevent damage or injury from the falling ball bearing.
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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.
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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.
Young’s Modulus (PAG)
Method and Calculations
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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.
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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.
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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.
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Calculate stress and strain:
- Use the results to calculate stress and strain of the wire.
- Plot a stress-strain curve.
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Analysis (y = mx + c)
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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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.
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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.
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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.
Resistivity (PAG)
Method and Calculations
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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).
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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.
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Repeat for different lengths:
- Reposition the flying lead for different wire lengths and repeat the process.
- Record the mean resistance for each length.
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Analysis (y = mx + c)
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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.
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Determine resistivity:
- Calculate ρ = gradient × A, where A is the cross-sectional area.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Avoid overheating by ensuring the circuit is set up correctly.
- Handle the wire carefully to prevent injury.
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Limitations:
- The wire may not have a perfectly circular cross-section, affecting area calculations.
- Temperature changes may alter the wire’s resistance.
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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.
Potential divider (PAG)
Method and Calculations
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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.
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Record data:
- Gradually heat the beaker, recording the temperature and voltage at regular intervals over a suitable range.
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Plot a graph:
- Plot voltage (y-axis) against temperature (x-axis).
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Analysis (y = mx + c)
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Handle the hot water carefully to avoid burns.
- Use a heat-resistant beaker and place it on a stable surface.
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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.
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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.
Diffraction grating (PAG)
Method and Calculations
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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.
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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).
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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.
- Use the formula: nλ = d sinθ, where:
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Analysis (y = mx + c)
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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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.
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Limitations:
- The small angle approximation may introduce errors for larger angles.
- The diffraction grating may have imperfections, leading to less distinct fringes.
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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.
Plank constant (PAG)
Method and Calculations
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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.
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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.
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Repeat and average:
- Repeat the experiment multiple times, averaging the results for V₀.
- Perform the experiment for a range of LEDs with different wavelengths.
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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.
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Calculate Planck constant (h):
- Use the gradient to calculate h = (gradient × e) / c.
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Analysis (y = mx + c)
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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.
- The equation eV₀ = hc/λ corresponds to y = mx + c, where:
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Determine Planck constant (h):
- Substitute the gradient into the equation h = (gradient × e) / c.
Accuracy, Safety, Limitations, and Improvements
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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.
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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.
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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.
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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.
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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.
Internal resistance (PAG)
Method and Calculations
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Set up the circuit:
- Set the variable resistor to its highest resistance.
- Record the current (I) and potential difference (V) across the circuit.
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Repeat measurements:
- Adjust the load resistance and repeat the measurements for multiple values.
- Calculate the mean current and voltage for each resistance.
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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.
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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.
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Analysis (y = mx + c)
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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.
- The equation V = E - Ir corresponds to y = mx + c, where:
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Determine internal resistance and e.m.f.:
- The gradient gives the internal resistance (r).
- The y-intercept gives the e.m.f. (E).
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Accuracy, Safety, Limitations, and Improvements
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Systematic Errors:
- Close the switch briefly to take readings, preventing changes in the internal resistance of the battery.
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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.
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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.
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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.
Oscilloscope (PAG)
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.
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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.
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Wave Properties:
- Oscilloscope traces can be used to calculate:
- Frequency: 1 ÷ period
- Period: Measured using the timebase.
Polarising filters for light (PAG)
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.
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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.
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Applications:
- Polaroid sunglasses: Use polarising filters to block partially polarised light, reducing glare.
Speed of sound (PAG)
Method and Calculations
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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.
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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.
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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.
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Analysis
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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.
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Handle the tuning fork carefully to avoid injury or damage.
- Ensure the tube is stable to prevent spills or accidents.
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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.
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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.
Semi circle light rays (PAG)
Method and Calculations
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Set up the experiment:
- Place the glass block on paper and shine light from the ray box into the curved surface of the block.
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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.
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Calculate refractive index:
- Use the formula: n = (sin c)–1 to calculate the refractive index (n) of the glass block.
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Analysis
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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.
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Interpretation:
- A higher refractive index corresponds to a smaller critical angle, indicating greater bending of light.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Handle the glass block carefully to avoid breakage or injury.
- Avoid shining the light directly into eyes.
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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.
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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.
Center of mass (PAG)
- Hang an object from a single point; the centre of mass will lie directly below that point.
- Hang the object from two different points and draw a plumb line (a vertical line) from each point.
- The intersection of these two lines is the centre of mass.
Specific Heat Capacity (PAG)
Measuring Specific Heat Capacity
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Measure initial conditions:
- Measure the mass (m) and initial temperature (T₁) of the substance.
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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.
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Calculate energy supplied:
- Use the formula: E = V × I × t.
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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
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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.
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Calculate specific heat capacity:
- Use the formula: m₁c₁(T₁ - T₀) = m₂c₂(T₀ - T₂).
- Rearrange to find the unknown specific heat capacity (c₁ or c₂).
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Analysis
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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).
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Assumptions:
- No heat is lost to the surroundings in the mixing method.
- The heater is 100% efficient in the heating method.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Handle hot substances carefully to avoid burns.
- Ensure electrical equipment (e.g., heater) is properly insulated to prevent electric shocks.
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Limitations:
- Heat loss to the surroundings can affect results in both methods.
- The mixing method assumes no heat loss, which is not always realistic.
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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.
Specific Latent Heat (PAG)
Method and Calculations
Measuring Specific Latent Heat of Fusion
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Set up the experiment:
- Use a heating coil in one funnel of ice.
- Connect the coil to an ammeter and voltmeter.
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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.
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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).
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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
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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.
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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.
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Calculate energy transferred:
- Use the formula: W = VIt.
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Calculate latent heat of vaporisation:
- Use the formula: L = E/m, where E is the energy transferred and m is the mass lost.
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Analysis
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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.
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Key equations:
- For fusion: E = mLf.
- For vaporisation: E = mLv.
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Accuracy, Safety, Limitations, and Improvements
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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.
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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.
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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.
Boyle’s Law (PAG)
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.
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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.
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Repeat and average:
- Repeat the experiment and calculate the mean for each reading.
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Analysis
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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.
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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Safety Considerations:
- Avoid over-pressurising the system to prevent the tube or gauge from bursting.
- Handle the tyre pump carefully to avoid injury.
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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.
Absolute Zero (PAG)
Method and Calculations
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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).
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Record initial conditions:
- Record the temperature of the water and the pressure on the Bourdon gauge.
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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.
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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.
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Analysis
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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.
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
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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.
Circular Motion (PAG)
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.
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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.
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Measure time period:
- Record the time (T) for one complete circle or multiple circles for greater accuracy.
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Calculate angular speed:
- Use the formula: ⍵ = 2π/T.
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Calculate centripetal force:
- Use the formula: F = m⍵²r, where m is the mass of the bung.
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Analysis
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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).
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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.
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Accuracy, Safety, Limitations, and Improvements
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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.
SHM (PAG)
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.
Capacitors in Series and Parallel (PAG)
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.
- Compare the experimental total capacitance (from the gradient) with the theoretical values for capacitors in series and parallel:
-
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.
Investigating Charging and Discharging Capacitors (PAG)
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.
Magnetic Flux Density (PAG)
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.
Magnetic Flux (PAG)
Method and Calculations
-
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.
-
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.
-
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.
-
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.
-
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.
-
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.
Transformers (PAG)
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.
Terminal Velocity in Fluids
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.
Ripple Tank (PAG)
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:
-
Wave Visualization:
- Bright bands on screen represent wave crests
- Enables direct measurement of wavelength (λ)
- Clear observation of wavefronts and their behavior
-
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
-
Reflection:
===
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)
Alpha, Beta & Gamma Radiation (PAG)
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
- Geiger-Müller tube connected to counter
- Radioactive sources (α, β, γ) - clearly labeled
- Test materials (paper, aluminum, lead sheets of varying thicknesses)
- 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)
- 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)
-
Quantitative Analysis:
- For γ radiation:
- Measure count rate through lead sheets (0.5mm to 10mm thickness)
- Plot absorption curve (count rate vs thickness)
- For γ radiation:
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
- Not accounting for dead time in GM tube at high count rates
- Inconsistent source-detector alignment
- Neglecting to subtract background from all measurements