Here are 2 schematics of exactly the same thing ... A capacitor, resistor, and inductor met at a node .. (fill in your own punchline). \(Z\) is the symbol for impedance now and \(Z_R\) has been used to designate the impedance due to a resistor. Initially, as the water wheel has mass, it does not turn (that is, it opposes the force of the pump). Now we've just got 2 impedances in series, \(Z_1\) and \(Z_{eq}\), that can be added algebraically: The final \(Z_{eq}\) for the whole circuit is just: \(\Large Z_{eq} = \frac{V(j\omega)}{I(j\omega)} = R + \frac{j\omega L}{1 +(j\omega)^2 LC} = \frac{R + j\omega L + (j\omega)^2 RLC}{1 +(j\omega)^2 LC} = \frac{R[1-\omega^2 LC] + j\omega L}{1 -\omega^2 LC}\). Consider the pressure profile in Figure 1. For any circuit, fluid or electric, which has multiple branches and parallel elements, the flowrate through any cross-section must be the same. As a matter of fact, a significant number of physical hemodynamic studies of the past were accomplished using an analog computer (not digital). We saw in the last article that it is mathematically acceptable to divide, multiply, add, and subtract sinusoids of the same frequency. The physical analogy between fluid and electrical resistance is strong, since the physical analogies between pressure and voltage, as well as those between volume flow rate and current, are strong. What we find is that the combination of these elements into circuit networks results in complicated behavior that can be used to model a host of physical processes, including circulatory function. (If it did, you would see that time-varying pressure and flow signals look exactly the same with \(R\) as the proportionality constant.) Kirchoff's current law tells us that the flow through the 2 resistors is the same so \(\Delta p_2 = q R_2\). I'll warn you ahead of time that you won't see something like this in the circulation. Now I'm going to ask you to make a big leap of faith. The electrical analogy steady-state model of a GPRMS published in Ref. While subtle, something else has happened to this equation representing resistance; the pressure and flow got capitalized and \(j\omega\) got stuck in all over the place. Here's an arbitrary example problem. The latter shows explicitly that we get volume (e.g. Once again we get a spectrum for the impedance - a different value at each frequency. and yes, the constituitive equations for fluid flow have near-perfect electrical analogues (just as you have written out) at least to first order, when the fluid flow is subsonic and incompressible. The next useful item is called Kirchoff's Voltage Law which states that the net (directed) voltage change around any closed loop in the circuit is \(0\). We'll look at some lumped parameter circulatory models a little later. Design and Production © 2004, University of As \(\omega \rightarrow \infty\), the circuit starts to look like this: and we have the same thing - the resistor connected to ground and the whole circuit looks like the resistor alone. Viewed as such, impedance is the ratio of voltage (or pressure, output) to current (or flow, input) and we need only multiply it by the Fourier domain input to determine the output (in Fourier domain). And the equivalent impedance of this thing? First we'll cover co… The interpretation of the "arbitrary" integration constant, \(V_0\), is easier to see in this form. Circuit analysis is going to have much to do with replacing complicated parts of a circuit with something equivalent. \(\omega = 1/\sqrt{LC}\) causes an infinite current that bounces back and forth between the capacitor and the inductor and also results in infinite impedance of the circuit as a whole. Know why the two terms are used, although there has been some corruption in mechanical... 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