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/* Verilog-A large-signal model for a ohmic cantilever RF MEMS switchContent of OHMIC_CANTILEVER_RF_MEMS_SWITCH.va. Open-source code covered by BSD license.The Verilog-A large signal model can be used for operating point, small signal (AC, SP) and large signal (HB, PSS, QPSS) simulations, using ADS, SpectreRF or Qucs. It includeslarge-signal electromechanical effects, as well as small-signal Brownian and Johnson-Nyquist noise.
Electromechanical: C-V hysteresis, hold-down, self-actuation, displacement-compensated squeeze-film dampingNoise: Brownian noise, Johnson-Nyquist noise (not included: 1/f noise)23th of July, 2011K. Van Caekenberghe (email@example.com)Check for update: http://www-personal.umich.edu/~vcaeken Reference: "RF MEMS Theory, Design and Technology", by G. M. Rebeiz, Wiley, 2003 */`include "disciplines.vams"`include "constants.vams"module OHMIC_CANTILEVER_RF_MEMS_SWITCH(s,d,g); inout s, d, g; electrical s, d, g; kinematic z, velocity; // Dimensions parameter real g_0=0.6e-6 from (0:inf); // nominal gap height [m] parameter real g_d=0.2e-6 from (0:inf); // nominal gap height minus dimple thickness [m] parameter real l=75e-6 from (0:inf); // beam length [m] parameter real t=5e-6 from (0:inf); // beam thickness [m] parameter real w=30e-6 from (0:inf); // beam width [m] parameter real W_c=10e-6 from (0:inf); // contact width [m] parameter real W=10e-6 from (0:inf); // electrode width [m] parameter real x=30e-6 from (0:inf); // beam anchor to electrode edge distance [m] // Electrical parameters parameter real R_c=1.0 from [0:inf); // contact resistance [Ohm] // Material parameters: beam (gold) parameter real rho=19.2e3 from (0:inf); // mass density [kg/m^3] parameter real E=78e9 from (0:inf); // Young's modulus [Pa] // Material parameters: gas (air): parameter real lambda=1.5e-7 from [0:inf); // mean-free path [m] parameter real mu=1.845e-5 from (0:inf); // viscosity coefficient [kg/(m.s)] // van der Waals and nuclear force coefficients parameter real c_1=10e-80 from [0:inf); // van der Waals force coefficient [N.m] parameter real c_2=10e-75 from [0:inf); // nuclear force coefficient [N.m^8] real A, b, C_ds, C_gs, C_u, F_c, F_e, F_s, f_m_0, I1, I2, IIP3, k_1, m, Q_e, Q_m, t_s_max, t_s_min, V_H, V_P, V_S; analog begin @ ( initial_step ) begin A=W*w; $strobe("\n%M: A (electrode area [m^2]) = %E",A); m=0.4*rho*l*t*w; $strobe("%M: m (effective beam mass [kg]) = %E",m); k_1=2*E*w*pow(t/l,3)*(1-x/l)/(3-4*pow(x/l,3)+pow(x/l,4)); $strobe("%M: k_1 (spring constant [N/m]) = %E",k_1); V_H=sqrt(2*k_1*(g_0-g_d)*pow(g_d,2)/(`P_EPS0*A)); $strobe("%M: V_H (hold-down voltage [V]) = %E",V_H); V_P=sqrt(8*k_1*pow(g_0,3)/(27*A*`P_EPS0)); $strobe("%M: V_P (pull-in voltage [V]) = %E",V_P); f_m_0=sqrt(k_1/m)/(2*`M_PI); $strobe("%M: f_m_0 (mechanical resonant frequency [Hz]) = %E",f_m_0); Q_m=(sqrt(E*rho)*pow(t,2)*pow(g_0,3))/(mu*pow(w*l,2)); $strobe("%M: Q_m (mechanical quality factor [) = %E",Q_m); V_S=V_P; t_s_max=27*pow(V_P,2)/(4*2*`M_PI*f_m_0*Q_m*pow(V_S,2)); $strobe("%M: t_s_max (maximum switching time [s], V_S = V_P) = %E",t_s_max); t_s_min=3.67*V_P/(V_S*sqrt(k_1/m)); $strobe("%M: t_s_min (minimum switching time [s], V_S = V_P) = %E",t_s_min); C_u=1.4*`P_EPS0*W_c*w/g_0; $strobe("%M: C_u (up-state capacitance [F]) = %E",C_u); IIP3=10*log(2*k_1*pow(g_0,2)/(`M_PI*10e9*pow(C_u*50,2)))+30; $strobe("%M: IIP3 (third order intercept [dBm], C=C_u, delta_f < f_m_0, f=10 GHz, Z=50 Ohm) = %E",IIP3); end // b: damping coefficient [N.s/m] (displacement-compensated squeeze-film damping) Q_e=Q_m*pow(1.1-pow(g_d*tanh(Pos(z)/g_d)/g_0,2),1.5)*(1+9.9638*pow(lambda/(g_0-g_d*tanh(Pos(z)/g_d)),1.159)); $strobe("\n%M: Q_e (displacement-compensated mechanical quality factor [) = %E",Q_e); b=k_1/(2*`M_PI*f_m_0*Q_e); $strobe("%M: b (damping coefficient [N.s/m]) = %E",b); // Forces F_c=c_1*W_c*w/pow(g_d-g_d*tanh(Pos(z)/g_d)+1e-9,3)-c_2*W_c*w/pow(g_d-g_d*tanh(Pos(z)/g_d)+1e-9,10); $strobe("%M: F_c (attractive van der Waals and repulsive nuclear forces [N]) = %E",F_c); F_e=`P_EPS0*A*pow(V(s,g),2)/2*1/pow(g_0-Pos(z),2); //F_e=`P_EPS0*A*pow(V(s,g),2)/2*1/pow(g_0-g_d*tanh(Pos(z)/g_d),2); // Envelope simulation $strobe("%M: F_e (electrostatic force [N]) = %E",F_e); F_s=k_1*Pos(z); //F_s=k_1*g_d*tanh(Pos(z)/g_d); // Envelope simulation $strobe("%M: F_s (spring force [N]) = %E",F_s); // Nonlinear state-space description Pos(velocity):ddt(Pos(z))==Pos(velocity); Pos(z):ddt(Pos(velocity))==1/m*(-b*Pos(velocity)-F_s+F_e+F_c+white_noise(4*`P_K*$temperature*b, "BROWNIAN_NOISE")); C_ds=1.4*`P_EPS0*W_c*w/(g_0-Pos(z)); I1=ddt(C_ds*V(d,s)); I2=V(d,s)/R_c+white_noise(4*`P_K*$temperature/R_c, "JOHNSON_NYQUIST_NOISE_R_c"); if (Pos(z)<g_d) I(d,s)<+I1; else I(d,s)<+I2; C_gs=1.4*`P_EPS0*A/(g_0-Pos(z)); I(g,s)<+ddt(C_gs*V(g,s)); endendmodule