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Dr Norman Rhodes, BSc MSc PhD FIMechE CEng, is Divisional Director at Mott MacDonald, and head of Mott MacDonald's Simulation and Modelling Group. He is responsible for the application of flow simulation techniques to solve engineering design problems. He has been actively involved in CFD work for over 20 years. Major areas of work include fire and smoke control, complex ventilation system evaluation, and fluid dynamics of heat-exchange processes. Dr Rhodes is Chairman of the Institution of Mechanical Engineers 'Energy Transfer and Thermofluid Mechanics Group' and is Secretary of the Permanent International Association of Road Congresses (PIARC) working group on 'Fire and Smoke Control in Tunnels'.

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Figure 12.4 HDDA/GrACE distributed dynamic storage [9].

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You cannot select objects before the LENGTHEN command The command responds with the Select an object or [DElta/Percent/Total/DYnamic]: prompt Choose one of the following options: Select object: This is the default However, its purpose is to display the current measurements of the object This can help you to decide how to define the final length or angle of the object The current length is displayed at the command line, and the previous prompt is repeated DElta: Right-click and choose DElta Delta means the change, or difference, between the current and new length or included angle The option responds with the Enter delta length or [Angle] <00000>: prompt If you want to change an included angle, rightclick and choose Angle Then type the change in the included angle Otherwise, simply type the change in the length of the object A positive number increases the length or included angle.

The time-domain numerical integration method has in fact two major drawbacks: on the one hand the number of equations grows with the dimension of the circuit, even when the largest part of it is linear. On the other hand, all the circuit elements must have a time-domain constitutive relation in order for the equations to be written in time domain. It is well known that in many practical cases the linear part of nonlinear microwave circuits is large and that it is best described in the frequency domain; as an example, consider the matching and bias networks of a microwave ampli er. In particular, distributed elements are very dif cult to represent in the time domain. A solution to these problems is represented by the convolution method [12 17]. By this approach, a linear subcircuit is modelled by means of frequency-domain data, either measured or simulated; then, the frequency-domain representation is transformed into time-domain impulse response, to be used for convolution in the time domain with the rest of the circuit. In fact, this mixed time-frequency domain approach is somehow dual to the harmonic balance method, to be described in a later paragraph. In order to better understand the approach, a general scheme of time-frequency domain transformations for periodic and aperiodic functions is shown in Appendix A.2. The basic scheme of the convolution approach is based on the application of eq. (1.5), with the relevant impulse response, to the linear subcircuit. Let us illustrate this principle with our test circuit, where a shunt admittance has been added (Figure 1.6). Equation (1.13) becomes C dv(t) g v(t) + imax tgh dt imax + iy (t) + is (t) = 0 (1.30)

A negative number decreases the length or included angle Percent: Right-click and choose Percent At the Enter percentage length <1000000>: prompt, type in what percent of the original object you want the final object to be Amounts over 100 lengthen the object Amounts under 100 shorten the object You cannot change an included angle using this option Total: Right-click and choose Total At the Specify total length or [Angle] <10000)>: prompt, you can either choose the Angle suboption, as described for the Delta option, or use the default total-length option Either way, you enter the total angle or length you want DYnamic: Right-click and choose DYnamic This option lets you drag the endpoint of the object closest to where you picked it You can use an object snap to specify the new endpoint.

Note that (9.153) and (9.154) were employed in obtaining TC (n) in (9.107).

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