| Syllabus Details |
References |
You should be able to... |
| Section 15.5 - The Physics of the eye (past paper questions and solutions) and ear (past paper questions and solutions)- |
| 15.5.1 |
Physics of vision: Simple structure of the eye
The eye as an optical refracting system; including ray diagrams of image formation |
Pope pp 28-32
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- label a diagram of the eye and know the function of each part
- draw ray diagrams to represent the rays being refracted by the optical system (as in Pope)
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| 15.5.2 |
Sensitivity of the eye
Spectral response as a photodetector |
Pope pp 32-36 |
- diagrams on pages 32, 33and 35 should be known and understood- they have come up in questions in the past
- Maximum refaction occus at the air cornea interface - the lens only provides minor adjustments in focus. - know diagram too!
- depth of focus with a small pupil is large - little adjustment is needed for focusing at differenet object distances - lttle strain when viewing in bright light. The converse is true for a large pupil.- know diagram too!
- Rods and cones should be known in detail - learn the graphs on page 35 - you should be able to sketch them from memory with numbers on the axes.
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| 15.5.3 |
Spatial resolution
Explanation in terms of the behaviour of rods and cones |
Pope pp 36-32 |
- the diagram on page 36 should be known and understood
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| 15.5.4 |
Persistence of vision (excluding a physiological explanation) |
Pope pp 39-40 |
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| 15.5.5 |
Depth of field |
Pope pp 40 |
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| 15.5.6 |
Lenses
Properties of converging and diverging lenses; principal focus, focal length and power
Use of the equations:



where
f = the focal length (+ve for a convex lens and -ve for a concave one)
u = the distance of the object from the centre (pole) of the lens, called the object distance
v = the distance of the image from the centre (pole) of the lens, called the image distance (if the image is a virtual one this distance will be negative and the image will be on the same side of the lens as the object.
M = magnification
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Question 4b June 2000
Answer Q4b Jun 2000 |
You should recall that:
- a converging lens makes the rays come to a real focus (cross at a point) it is called a CONVEX lens
- a diverging lens makes the rays appear to be spreading out from a point on the opposite side of the lens (cross at a virtual point) it is called a CONCAVE lens
- The principal focus of a convex lens (sometimes called the focal point) it is the point on the principal axis, through which rays of light, travelling near to and parallel to the principal axis, pass after refraction by the lens.
- The principal focus of a concave lens (sometimes called the focal point) it is the point on the principal axis, from which rays of light, travelling near to and parallel to the principal axis, apear to diverge from after refraction by the lens. (they can be traced back through this point.
- The focal length of a lens is the distance between the pole of the lens and the principal focus. If the lens has a real focus then the focal length is positive. If it has a virtual focus it is negative.
- The power of a lens is the reciprocal of the focal length in metres. It is measured in dioptres (D). The sign of the power will be the same as the sign of the focal length.
You should be able to do calculations using the equations - care with signs! and units! |
| 15.5.7 |
Ray diagrams
Image formation |
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You should be able to construct the following diagrams
Convex lens: object at 2F, object between F and 2F, object at F , object between P and F and object beyond 2F
Concave lens: object at 2F, object between F and 2F, object at F and object between P and F
You MUST draw these properly - construct them! - sketches will not do!
Use a ruler and a sharp pencil.
Three basic rules to construc an image:
Rays that pass through the pole of the lens are undeviated.
Rays that are travelling parallel to and near to the principal axis pass through the principal focus after refraction by the lens (for a convex lens) and appear to emanate from the principal focus (draw in dotted lines) for a concave lens.
The converse is true, in that rays passing through (or emanating from) the principal focus emerge parallel on the other side of the lens. |
| 15.5.8 |
Defects of vision: myopia, hypermetropia and astigmatism |
Question 4a June 2000
Answer Q4a Jun 2000 |
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| 15.5.9 |
Correction of defects of vision using lenses
Ray diagrams and calculations of powers (in dioptres) of correcting lenses for myopia and hypermetropia
The format of prescriptions for astigmatism |
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| 15.5.10 |
Physics of hearing
Speed of sound in solid and gaseous media |
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| 15.5.11 |
Acoustic impedance Definitions of intensity and attenuation |
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| 15.5.12 |
The ear as a sound detection system: Simple structure of the ear, transmission processes |
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| 15.5.13 |
Sensitivity and frequency response
Production and interpretation of equal loudness curves
Human perception of relative intensity levels and the need for a logarithmic scale to reflect this |
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| 15.5.14 |
Relative intensity levels of sounds
Measurement of sound intensity levels and the use of dB and dBA scales |
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| 15.5.15 |
The threshold of hearing

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| 15.5.16 |
Defects of hearing
The effect on equal loudness curves and the changes experienced in terms of hearing loss of:
- injury resulting from exposure to excessive noise;
- deterioration with age (excluding physiological changes) |
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Noes on the Cyberphysics site - see table of problems with hearing |
Section 15.6 - Biological measurement and imaging -
fibre optics past paper questions and solutions
heart past paper questions and solutions
lasers papt paper questions and solutions
ultrasound past paper questions and solutions
X-ray past paper questions and solutions |
| 15.6.1 |
Basic structure of the heart. The heart as a double pump with identified valves
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Pope page 69/70 |
Note that full heart is not required but all in Pope is! |
| 15.6.2 |
Electrical signals and their detection
The biological generation and conduction of electrical signals;
methods of detection of electrical signals at the skin surface |
Pope chapter 5 (pp 67-73) |
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| 15.6.3 |
Action potentials The response of the heart to the action potential originating at the sino-atrial node |
Pope page 68-69 |
You need to KNOW the diagrams! |
| 15.6.4 |
Simple ECG machines and the normal ECG waveform
Principles of operation for obtaining the ECG waveform;
explanation of the characteristic shape of a normal ECG waveform |
Pope page 70-72 |
All of the detail here can be asked for in the exam! |
| 15.6.5 |
Ultrasound imaging: Reflection and transmission characteristics of sound waves at tissue boundaries, acoustic impedance
Advantages and disadvantages of ultrasound imaging in comparison with alternatives including safety issues and resolution
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Pope page 117-118
Pope page 130-131 |
Look to the notes on cyberphysics as well as your text book |
| 15.6.6 |
Piezoelectric devices: Principles of generation and detection of ultrasound pulses
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Pope page 118-119 |
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| 15.6.7 |
A-scan and B-scan Examples of applications |
Pope page 119-125 |
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| 15.6.8 |
Fibre optics and lasers
Properties of fibre optics and applications in medical physics; including total internal reflection at the core-cladding interface |
Pope pages109-113 |
Revise AS work and then see how it is applied here
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| 15.6.9 |
Endoscopy: Physical principles of the optical system of a flexible endoscope; the use of coherent and non-coherent fibre bundles; examples of use for internal imaging and related advantages |
Pope pages109-113 |
Revise AS wok and then see how it is applied here |
| 15.6.10 |
Properties of laser radiation
Absorption by tissue |
Pope pages 113-115 |
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| 15.6.11 |
Uses of lasers in medicine
Safety issues |
Pope pages 113-115 |
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| 15.6.12 |
X-ray imaging The physics of diagnostic X-rays |
Pope pages136 - 160 |
see cyberphysics notes too |
| 15.6.13 |
Physical principles of the production of X-rays:
- rotating-anode X-ray tube;
- methods of controlling the beam intensity,
- the photon energy,
- the image sharpness and contrast and
- the patient dose |
Pope pages 151-156 |
Important topic - make sure you know what each part does and why! |
| 15.6.14 |
Differential tissue absorption of X-rays (excluding details of the absorption processes) |
Pope pages 142-147 |
Note that you do NOT need details of the attenuation processes! |
| 15.6.15 |
Exponential attenuation Linear coefficient m, mass attenuation coefficient mm and half-value thickness x ( remember r is density!!)
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Pope pages 142-144 |
You did something similar with gamma ray absorption |
| 15.6.16 |
Image contrast enhancement: use of X-ray opaque material as illustrated by the barium meal technique |
Pope page 149 |
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| 15.6.17 |
Radiographic image detection
Photographic detection with intensifying screen and fluoroscopic image intensification; reasons for using these |
Pope page 148-151 |
Main reason for development of the intensifying screen etc. is to cut down on the dose of X-rays that has to be delivered. You need to use CALRAD to familiarize yourself with the procedures adopted to do this and the problems that can arise from ionizing radiation exposure.
Cellular damage (within one person) can lead on to systemic (passed on to offspring) damage. See here. |