Eduqas Physics Practicals for AS Physics1 1 Remember that the practicals may not
be exactly as below
Exeter Mathematics School
2 Jan 2017
This document covers the core practicals from the Eduqas AS physics specification. The practicals may be conducted with different methods, the important thing is to learn the principles, aims, and techniques, rather than the exact methods.
Measurement of the density of solids 2
Determination of unknown masses by using the principle of moments 2
Measurement of g by freefall 4
Investigation of Newton’s 2nd law 5
Determination of Young modulus of a metal in the form of a wire 6
Investigation of the force-extension relationship for rubber 7
I-V characteristics of the filament of a lamp and a metal wire at constant temperature 8
Determination of the internal resistance of a cell 9
Measurement of the intensity variations for polarisation 10
Determination of wavelength using Young’s double slits 11
Determination of wavelength using a diffraction grating 12
Determination of the speed of sound using stationary waves 13
Determination of resistivity of a metal 14
Investigation of the variation of resistance with temperature for a metal wire 16
Measurement of the refractive index of a material 17
Determination of h using LEDs 18
Measurement of the density of solids
The density of regularly shaped solids can be determined by measuring their mass, m, and calculating their volume, V. The density, ρ, can then be found using: m
Various regularly shaped solids both rectangular and circular,
30 cm ruler (resolution ±0.1 cm)
Vernier calipers / micrometer (resolution ±0.01 mm)
Balance (resolution ±0.1 g)
Determine the mass of the object using the balance. The volume of a rectangle can be found by measuring the length, l, width, w, and height, h. Calculate the volume, V using:
V = lwh
The volume of a sphere is found by measuring the diameter to find the radius, r, and then calculate the volume using:
V = πr3
2 Irregular shapes are harder to mea-
In both cases calculate the density using: ρ = m/V.
Determination of unknown masses by using the principle of moments
Apply the principle of moments to a metre rule to first determine its mass and then determine the mass of an unknown object.
Meter rule Clamp and stand
sure, so we use the Archimedian principle and a water displacement can to measure the volume. If faced with a buoyant object you can weigh it down with another object, so long as you subtract the volume of that weight from the total volume of water displaced.
Figure 1: Displacement can in use.
200 g mass and hanger
150 g mass (covered in tape and labelled as W) and hanger
Loops of thread
Now remove the 200 g mass and replace it with the unknown weight, W, and again adjust the position of the weight until the ruler balances. Measure the distance, d, of the unknown weight from the pivot. The unknown weight can again be calculated by applying the principle of moments:
The unknown weight can be converted into a mass (in kilograms) by dividing by 9.81. This can then be checked using a top pan bal-
|ance.3||3 better to use the term “Top-pan balance” than “scales”|
Loop a 200 g (1.96 N) mass over the metre rule and adjust it until the ruler is horizontal. Note down the distance, x, of the mass from the pivot. The mass (or weight) of the metre rule can now be calculated using the principle of moments:
Figure 2: Experimental set-up for the measurement of an unknown mass by moments. It would be possible to use a knife-edge fulcrum (pivot) instead
Measurement of g by freefall
An equation of motion can be used to calculate the acceleration due to gravity, g.4
4 There are two common alternative
methods to the one below.
s = ut +mv2 (1) 1. Manual timing - This method has a
lot of inherent errors, and gives poor
|Where : u = initial velocity = 0, s = height, h and a = acceleration due to gravity, g||
the approx 0.3 s it takes to start and
significant are usually parallax and
This gives h =gt2 (1) 2. Using lightgates - Lightgates are
very accurate, and a viable alterna-
If a graph of height, h, (y-axis) is plotted against time squared, t2, (x-axis) the gradient will equal g/2, or g = 2 × gradient.
All of these methods rely on the same basic equations of motion
Figure 3: “g” by freefall
When the switch is pressed it disconnects the electromagnet releasing the metal sphere5. At the same instant the timer starts. When the sphere hits the magnetic switch it breaks the circuit stopping the timer, thus recording the time it takes for the sphere to fall through a height, h. The time taken for the ball bearing to fall through a range of different heights needs to be measured. Plot a graph of height, h, (y-axis) against time squared, t2, (x-axis) and calculate the value of g using: g = 2/gradient.
Investigation of Newton’s 2nd law
The gravitational force of the slotted masses attached via the pulley causes the entire mass of the system to accelerate. That is the mass of the rider, M, and the total mass of the slotted masses, m. NewtonâA˘ Zs second law, therefore, can be written as:´
mg = (M + m)a
and so the acceleration of the system is:
(M + m)
We can use this to test Newton’s second law. If the total mass of the system (M + m) remains constant2 then the acceleration, a, should be
proportional to the gravitational force, mg.
reason that we take masses from the
hanger and place them onto the car and vice-versa
Figure 4: Newton’s law experiment. Note that an air-track is not strictly necessary, we’re trying to minimise the effect of friction on the system.
|Fix the thread to the rider and attach five slotted 5 gram masses to the other end as shown in the diagram. Set the light gates to record the acceleration and allow the slotted masses to fall to the ground. Record the gravitational force, mg and the acceleration, a. Remove one of the slotted masses and place it on the rider (so keeping the total mass of the system constant). Repeat the experiment until all the different accelerating masses have been removed. Plot a graph of acceleration (y-axis) against gravitational force, mg (x-axis). This|
|should be a straight line through the origin. 7||7 By using a scales to measure the combined mass of the system M+, m you could check that the gradient is|
Determination of Young modulus of a metal in the form of a wire
Young modulus = StrainStress or E = Fx//Al rearranging E = xAFl where:
F = applied load (7)
If a graph of applied load, F (y-axis) is drawn against extension, x (x-axis) the gradient is Fx and so:
The original length l can be measured and the area of the wire found using A = πr2 hence E can be determined.
Hang two identical wires from a beam and attach a scale to the first
|equal to 1/(M + m)|
|wire and a small weight to keep it straight.8 Also put a small weight||8 We use this method to eliminate any|
|on the second wire to straighten it and a Vernier scale linking with the scale on the comparison wire. Measure the original length, l, of||thermal extension/contraction|
|the test wire and its diameter at various points along its length9. Use||9 Measuring at several places along the|
|this to calculate the mean cross sectional area A. Then place a load of 5 N on the test wire and find the extension, x. Repeat this in 5N steps up to at least 50N. Plot a graph of load (y-axis) against extension (x-axis) and calculate the gradient. Use this to find a value for the Young modulus.||length is a favourite of exam boards.|
Figure 5: Young’s Modulus apparatus
Investigation of the force-extension relationship for rubber
Rubber is an example of a polymer with weak cross bonds. Natural rubber is a polymer of the molecule iso-prene. It has weak van der Waals cross-bonds and only a few covalent (strong) cross-bonds.
Rubber band of cross-section approximately 1 mm by 2 mm
Clamp and stand G-clamp to secure (if required) 50 g mass holder plus a number of 50 g masses
Optical pin (for use as a pointer if required)
Metre rule (resolution ±0.001m) Micrometer (resolution ±0.01mm)
Hang a (cut) rubber band of (approximate) cross-section 1 mm by 2
mm vertically from a stand, boss and clamp. The base of the stand should be secured using a G-clamp. Hang a 50 gram mass holder from the band. Place a metre rule as close as possible to the mass holder. The length can be read using an optical pin attached to the base of the mass holder. Measure the length, width and thickness of
Figure 6: Hysteresis graph for rubber band
the rubber when it is supporting the 50 gram holder. Try to avoid squashing the rubber with the micrometer screw gauge. Increase the mass in 50 gram steps, measuring the extension each time. Continue until the band breaks.10 Plot the force - extension curve and
10 If, instead of testing to failure, you
determine the Young modulus from the linear section.
I-V characteristics of the filament of a lamp and a metal wire at con-
now unload the masses and measure the extension you can measure the elastic hysteresis - the work done in rearranging the internal structure of the rubber.
Ohm’s law states that for a conductor the current, I, is directly proportional to the potential difference, V, provided physical factors such as temperature and pressure remains constant. Therefore by plotting the I-V characteristic of each of, a metal wire and a filament lamp, the validity of Ohm’s law as applicable to each of these components can be determined. A graph of I against V is linear for a metal wire and non-linear for a filament of a lamp.
Variable d.c. voltage supply
Component either in the form of a filament bulb e.g. 12 V, 24 W bulb or a metal wire e.g. 1 m length of constantan mounted on a wooden batten
The circuit should be set up as in figure 8.
Starting with the output of the variable d.c. voltage supply set to its minimum value, slowly increase the value of the applied voltage. The current through the component and the potential difference across the component should be recorded for a range of values of the applied voltage. A graph of current against voltage should then be plotted. This procedure can be repeated for different components.
Figure 7: VI graphs of common components
Figure 8: V-I Characteristics set-up.
Note the variable powersupply and the switch. This basic circuit is used
to investigate almost every electrical component
|Determination of the internal resistance of a cell Theory:|
|11When charge flows through a cell it is given energy by the cell.||11 I’ve tried to be quite clear here and|
|The number of joules of energy given to each coulomb of charge that passes through the cell is the e.m.f.12 of the cell. The energy can only be transferred to the charges at a finite rate, we model this as the cell having resistance. This model resistance is called the internal||
give a bit of extra detail. Internal resistance is a favourite of examiners and I’d be amazed if this experiment didn’t show up in some way
12 e.m.f. is an abbreviation for electromotive force.
resistance of the cell. A cell can be thought of as a source of e.m.f.
with a resistor connected in series.
When current flows through the cell a voltage develops across the internal resistance. This voltage is not available to the circuit so it is called the lost volts, (VL). VL can also be written as Ir The voltage across the ends of the cell is called the terminal potential difference,
(Vt.p.d). Vt.p.d can also be written as IR Because voltage is a measure of energy, and energy is always conserved, the e.m.f. of a cell is equal to the sum of its terminal potential difference, (Vt.p.d), and the lost volts, (VL). This gives rise to the equation:
E = Vt.p.d. + VL
This equation can be written in different forms, e.g. E = I(R + r)
The most common form of the equation used for determining the internal resistance is V = E − Ir where V is the terminal p.d. of a cell; E is the emf of the cell; I the current flowing in the circuit and r is the internal resistance. V = IR and the equation can be re-written
Figure 9: Internal resistance graph
as R = EI − r. Therefore a graph of R against 1/I should be linear.
Cells - e.g. 3 or 4 1.5 V ‘D’ type batteries connected in series
Ammeter or multimeter set to A range - ±0.01 A
Various resistor values 0 Ω to 60 Ω
The circuit should be set-up as follows:
The resistor values should be varied and the current values recorded. Plot a graph of R (y-axis) against 1/I (x-axis). The graph should be a straight line with the intercept on the y-axis which is equal to the value of the internal resistance.
Measurement of the intensity variations for polarisation
The light waves in a ray of light from a lamp have vibrations in all planes and directions. The light is unpolarised. When the light passes through a polaroid filter; the vibrations will be in one plane or direction only. In the experiment with two pieces of polaroid, the first polarises the light. The light will then not pass through the second polaroid if the direction in which the second filters polarises light is at right angles to the polarising direction of the first polaroid.
Two pieces of polaroid
Lamp e.g. 24 W, 12 V bulb in holder
Investigate the variation in intensity by looking through the lamp through both polaroids and rotating one of the polaroids through 360°. Note the change in intensity that occurs.
Figure 10: Investigating the Polarisation
Determination of wavelength using Young’s double slits
Young’s interference experiment, also called Young’s double-slit interferometer, was the original version of the modern double-slit experiment, performed at the beginning of the nineteenth century by Thomas Young. This experiment played a major role in the general acceptance of the wave theory of light. The fringe spacing, ∆y is given by the equation∆y = λdD where λ is the wavelength of the light; D is the distance from the slits to the screen where the fringes are viewed and d is the distance between the slits. A graph of ∆y against D should be a straight line and the gradient can be used to determine the wavelength of the light.
Stand and clamp
of light. When the full version (not on the spec) is done, the intensity of light and the angle of the analyser relative to the polariser is measured. The experiment is used to test malus’s law. According to malus, when completely plane polarized light is incident on the analyzer, the intensity of the light transmitted by the analyzer is directly proportional to the square of the cosine of angle between the transmission axes of the analyzer and the polarizer.
30 cm ruler or digital callipers
The apparatus should be set-up as follows:
∆y, the spacing between the slits, d, and the distance, D, from the slits to the screen using either the ruler or digital callipers. Vary the distance, D in equal intervals. Plot a graph of the fringe spacing ∆y (y-axis) against the slit-screen distance D (x-axis). This should be a straight line through the origin. If the fringes are close together;
Figure 12: Fringe pattern for red light of 633 nm.
∆y can be determined by measuring the separation of a number of fringes. So determine by dividing the distance by the number of fringes measured.
Determination of wavelength using a diffraction grating
The diffraction grating equation is given by nλ = d sin θ. The spacing between the lines in a diffraction grating is usually specified or can be found from the grating ruling.
By measuring the angle θ, the wavelength of the light can be determined.
Diffraction grating of known d value or ruling e.g. 300 lines cm−1
Figure 13: Geometry of diffraction
Stand and clamp for laser and grating
The apparatus should be set-up as follows: The value of θ can be
Figure 14: Diffraction grating setup
determined from tan θ = Dx .
Using the equation nλ = d sin θ then the wavelength can be determined for various orders of diffraction.
Determination of the speed of sound using stationary waves
When resonance first occurs the length of air in the tube, l, plus a small end correction, e (to account for the position of the tuning fork above the tube) will be equal to a quarter of a wavelength. Hence:
l + e = λ/4
but λ = c/f
l = − e
If a graph is plotted of l (y-axis) against 1/f (x-axis) it should be a straight line with a small negative y-intercept.
The gradient of the graph equals c/4, and so the speed of sound, c, can be found. The small negative intercept will give the end correction.
A range of at least five different tuning forks will be needed along with a metre ruler of resolution ±0.001 m.
Figure 15: Standing waves in an open ended pipe
Initially place the resonance tube as deep as possible into the water. Then gradually raise it. As this is being done hold a vibrating tuning fork over the top. When resonance occurs (a loud sound will be heard) measure the length of the tube above the water level. Repeat the above for each of the tuning forks. Plot a graph of length (y-axis) against 1/frequency (x-axis). Use the gradient to determine a value for the speed of sound.
Determination of resistivity of a metal
13 There are lots of possible experiments
here. So long as you are systematic in changing only one variable in R = ρl
Resistivity, ρ can be found using the equation R = ρAl where l is the length of the wire, A the cross-sectional area and R the resistance.
This can be compared with the equation for a straight-line y = mx + c. A graph plotted of R (y-axis) against l (x-axis) will be a straight line through the origin of gradient Aρ . The cross sectional area can be found using A = πr2 and the resistivity calculated by ρ = gradient × A.
Figure 16: Geometry of resistivity
Figure 17: Experimental set-up for Resistivity of a wire investigation
1.5 V ‘D’ type battery
110 cm length of nichrome wire
1 micrometer / vernier callipers (resolution ±0.01 mm)
30 cm ruler (resolution ±0.001 m)
Leaving one crocodile clip fixed at one end of the wire, the other clip should be moved along at suitable intervals e.g. every 10 cm / 20 cm to cover the whole range of the wire. Readings on the voltmeter and ammeter should be noted for each length and the resistance determined using R = VI . The diameter of the wire can be found using a micrometer or Vernier callipers and the cross-sectional area determined. Plot a graph of R (y-axis) against l (x-axis) and calculate the resistivity using: ρ = gradient × A.
Investigation of the variation of resistance with temperature for a metal wire Theory:
|Resistance increases with temperature for metals in a linear relationship. This practical will enable data to be obtained to investigate this|
|relationship. 14.||14 A common substitution is to swap the wire in the investigation for a thermistor. Thermistors are semicon-|
|ductor devices that have the reversed behaviour to normal wires. As their temperature increases, the resistance of a thermistor decreases|
|• Ice||Because the effect of resistance change with temperature is small, it is im-|
The circuit should be set up as follows: The water bath should be
|portant to cover as large a range of temperatures as is safe and practical. In an A-level lab it would be possible to get down to about −40 °C and up to about 1200 °C. These extreme temperatures are dangerous however and would need particular precautions|
Figure 18: Resistance of a wire with Temperature
heated and the water stirred continuously in order to ensure an even
temperature throughout the water bath. Once the required temperature has been reached then remove the heat and record the reading of resistance or take the ammeter and voltmeter readings. This process should be repeated at intervals until the water boils. Repeat the experiment during cooling. Plot a graph of resistance (y-axis) against temperature (x-axis). This should be a straight line through the origin. An ice water mixture can be used to record the resistance at a temperature of 0 °C.
Measurement of the refractive index of a material
The refractive index, n, of a material can be determined from the equation sin θi = sin θr where n = refractive index, θiis the angle of incidence and θr is the angle of refraction.
The above equation assumes that the incident ray is travelling in air. A graph of sin θi (y-axis) against sin θr (x-axis) will give a straight line through the origin and the gradient is equal to the refractive index, n.
• Suitable white light source e.g. ray box fitted with a single slit to
Figure 19: Refractive index measurement
plotted which should give a straight line. A value of n can then be determined from the gradient.
surface. In this case it is at 90° to the glass block, as shown by a dotted line in the diagram
Determination of h using LEDs
The Planck constant, h, can be determined by using a light emitting diode (LED) and measuring the minimum voltage, Vmin, at which light is just emitted by the diode. 17 The Planck constant can then
17 The energy levels in the LED are
be determined from the equation Vmin = ehcλ where c is the speed of light 3.00 × 108 ms−1 and e is the electronic charge, 1.60 × 10−19 C. A graph of Vmin against 1/λ should be a straight line with the gradient equal to V
Variable d.c. power supply
1 kΩ protective resistor
Voltmeter (resolution ±0.01 V) [multimeter set to appropriate range]
Various LEDs - with known wavelengths
The circuit should be set-up as follows:
quantised, and they are constructed such that their emissions are monochromatic. Because energy is conserved, the only light that the LED can emit will have an energy corresponding to the energy level transition inside the material.
Potential difference is a measure of the energy difference between two points. The potential required to light the LED must therefore be the energy of the photons released. Photon energy is given by E = hf, where h is planck’s constant and f is the frequency of light.
18 Many experiments have equations in the form y = mx + c. You should expect to have to match the variables in an equation with the parts of an equation of a straight line. It would be unsurprising to have a question requiring you to calculate gradients and
The voltage should be varied until light is just emitted by the LED. Record the voltage it corresponds to Vmin. The LED should be replaced and the procedure repeated for LEDs with different wavelengths of light. Plot a graph of Vmin (x-axis) against 1/λ (y-axis) and use it to determine a value for h.