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Introduction to Sports Biomechanics: Analysing Human Movement ...

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Recorders<br />

Frequency response<br />

The ability of the amplifier <strong>to</strong> reproduce the range of frequencies in the signal is known<br />

as its frequency response. The required frequency response depends upon the frequencies<br />

contained in the EMG signal. This is comparable with the requirement for audio<br />

amplifiers <strong>to</strong> reproduce the range of frequencies in the audible spectrum. Typical values<br />

of EMG frequency bandwidth are 10–1000 Hz for surface electrodes and 20–2000 Hz<br />

for indwelling electrodes. Most modern EMG amplifiers easily meet such bandwidth<br />

requirements. About 95% of the EMG signal is normally in the range up <strong>to</strong> 400 Hz,<br />

which explains why SENIAM recommend the use of a low-pass filter <strong>to</strong> remove higher<br />

frequencies. This signal range unfortunately also contains mains hum at 50 or 60 Hz.<br />

Also, SENIAM recommends that the input-referred voltage and current noise, respectively,<br />

should not exceed 1 µV and 10 pA.<br />

Common mode rejection<br />

THE ANATOMY OF HUMAN MOVEMENT<br />

Use of a single electrode would result in the generation of a two-phase depolarisation–<br />

repolarisation wave (Figure 6.21). It would also contain common mode mains hum.<br />

At approximately 100 mV, the hum is considerably larger than the EMG signal. This is<br />

overcome by recording the difference in potential between two adjacent electrodes,<br />

known as bipolar electrodes, using a differential amplifier. The hum is then largely<br />

eliminated as it is picked up commonly at each electrode because the body acts as<br />

an aerial – hence the name ‘common mode’. The differential wave becomes triphasic (it<br />

has three phases, as in Figure 6.21). The smaller the electrode spacing, the more closely<br />

does the triphasic wave approximate <strong>to</strong> a time derivative of the single electrode wave. In<br />

practice, perfect elimination of mains hum is not possible and the success of its removal<br />

is expressed by the common mode rejection ratio (CMRR). This should be 10 000 or<br />

greater. The overall system CMRR can be reduced <strong>to</strong> a figure lower than that of the<br />

amplifier by any substantial difference between the two skin plus cable resistances. The<br />

effective system common mode rejection ratio in this case can be downgraded <strong>to</strong> a value<br />

of R i/(R 1 − R 2); cables longer than 1 m often exacerbate this problem. For passive<br />

electrodes, the attachment of the pre-amplifier <strong>to</strong> the skin near the electrode site reduces<br />

noise pick-up and minimises any degradation of the CMRR arising from differences<br />

between the cable resistances.<br />

Various devices have been used his<strong>to</strong>rically <strong>to</strong> record the amplified EMG signal but at<br />

present A–D conversion and computer processing are by far the most commonly used<br />

recording methods. An A–D converter with 12-bit (1 in 4096) or 16-bit resolution is<br />

recommended by SENIAM. High sampling rates are needed <strong>to</strong> reproduce successfully<br />

the signal in digital form; telemetered systems do not always provide a sufficiently high<br />

sampling rate.<br />

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