Page 136 - Biomedical Engineering and Design Handbook Volume 1, Fundamentals
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BIOMECHANICS OF THE RESPIRATORY MUSCLES  113

                          a device with a weighted plunger, which requires development of enough pressure to lift the plunger
                          out of its socket in order to initiate inspiration (Nickerson and Keens, 1982). The endurance is
                          expressed as the time the subject can endure a particular load or as the maximum load tolerated for
                          a specific time (Fiz et al., 1998). In the resistive inspiratory load the subject breathes against a vari-
                          able inspiratory resistance at which the subject had to generate a percentage of his maximal mouth
                          pressure in order to inspire. Endurance is expressed as the maximal time of sustained breathing
                          against a resistance (Reiter et al., 2006; Wanke et al., 1994). The postinterruption tracing of mouth
                          pressure against time represents an effort sustained (against an obstructed airway) over a length
                          of time and can serve as a pressure-time index of respiratory muscle endurance. The area under this
                          tracing (i.e., the pressure-time integral) represents an energy parameter of the form PT, where P is
                          the mean mouth pressure measure during airway obstruction and T is the time a subject can sustain the
                          obstruction (Ratnovsky et al., 1999). Similar to the strength of respiratory muscles, large dependence
                          on lung volume was found for their endurance. The endurance of expiratory muscles decreased as
                          lung volume decreased from TLC, while the endurance of inspiratory muscles decreased as lung volume
                          increased from RV (Ratnovsky et al., 1999).


              5.3.3 Electromyography
                          Electromyography (EMG) is a technique for evaluating the electrical activity of skeletal muscles at
                          their active state (Luca, 1997). Intramuscular EMG signals are measured by needle electrodes inserted
                          through the skin into the muscle, while surface EMG signals are recorded with surface electrodes
                          that are placed on the skin overlying the muscle of interest. Typically, EMG recordings are obtained
                          using a bipolar electrode configuration with a common ground electrode, which allows canceling
                          unwanted electrical activity from outside of the muscle. The electrical current measured by EMG is
                          usually proportional to the level of muscle activity. Normal range for skeletal muscles is 50 μV to
                          5 mV for a bandwidth of 20 to 500 Hz (Cohen, 1986).
                            The raw EMG data resembles a noise signal with a distribution around zero. Therefore, the data
                          must be processed before it can be used for assessing the contractile state of the muscle (Herzog,
                          1994). The data can be processed in the time domain or in the frequency domain. The EMG signal
                          processing in the time domain includes full wave rectification in which only the absolute values of
                          the signal is considered. Then in order to relate the EMG signal to the contractile feature of the mus-
                          cle it is desired to eliminate the high-frequency content by using any type of low-pass filter that
                          yields the linear envelope of the signal. The root-mean-square (RMS) value of the EMG signal is an
                          excellent indicator of the signal magnitude. RMS values are calculated by summing the squared values
                          of the raw EMG signal, determining the mean of the sum, and taking the square root of the mean

                                                            tT
                                                             +
                                                           1
                                                    RMS =  T ∫  EMG 2 ()tdt                   (5.1)
                                                             t
                            The study of EMG signals in the frequency domain has received much attention due to the loss
                          of the high frequency content of the signal during muscle fatigue (Herzog, 1994). Power density
                          spectra of the EMG signal can be obtained by using fast Fourier transformation technique. The most
                          important parameter for analyzing the power density spectrum of the EMG signal is the mean fre-
                          quency or the centroid frequency, which is defined as the frequency that divides the power of the
                          EMG spectrum into two equal areas.


              5.3.4 Electromyography of the Respiratory Muscles
                          Using EMG for assessment of respiratory muscles performance, in addition to the methods described
                          in the above paragraphs, enables differentiation between different respiratory muscles. The EMG
                          signals can detect abnormal muscle electrical activity that may occur in many diseases and conditions,
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