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. Author manuscript; available in PMC: 2016 Aug 1.
Published in final edited form as: Laryngoscope. 2015 May 22;125(8):1892–1899. doi: 10.1002/lary.25267

Table 1.

Ranges of objective functions (F0, SPL, subglottal pressure) and decision variable (μ1) used for optimized simulation. Other parameters were kept constant. Three surgeries were simulated (see Figure 1). The subscripts denote the layer specified: layer 1: normal SLLP or scar; layer 2: ligament; layer 3: muscle; layer 4: implant. The material in the FEM was considered as a fiber-gel compound, fiber-like along the vocal fold longitudinally, but gel-like in the coronal plane, i.e. transversally isotropic. The longitudinal shear moduli of SLLP, ligament, and muscle were designated as μ1,μ2, and μ3, respectively. The transverse shear moduli of SLLP, ligament, and muscle were designated as μ1, μ2, and μ3, respectively, and reflect the gel properties. Viscosity is designated by η1, η2, and η3. For the scar layer, μ1 would increase with greater deposition of organized collagen in the longitudinal orientation. Since collagen fibers are randomly organized in scar45, μ1 was not altered. The lower boundary of μ1 was increased 3-fold to account for the higher collagen fiber content in scar. This was based on the observation that scarred vocal fold tissue demonstrates a smaller range for μ with an increased lower limit.46

Normal vocal fold Subepithelial Transligamental Subligamental
F0 (Hz) 120 (90–150) 120 (90–150) 120 (90–150) 120 (90–150)

SPL (dB) 70 (60–80) 70 (60–80) 70 (60–80) 70 (60–80)

Subglottal pressure (kPa) 0.01 to 2 0.01 to 2 0.01 to 2 0.01 to 2

μ′1 (dyn/cm2) 5000 5000 5000 5000

μ′2 (dyn/cm2) 20000 20000 20000 n/a

μ′3 (dyn/cm2) 15000 15000 15000 15000

μ′4 (dyn/cm2) n/a 500000 500000 500000

μ1 (dyn/cm2) 5000–50000 15000–50000 15000–50000 15000–50000

μ2 (dyn/cm2) 5000 5000 5000 n/a

μ3 (dyn/cm2) 5000 5000 5000 5000

μ4 (dyn/cm2) n/a 500000 500000 500000

η1 (poise) 2 2 2 2

η2 (poise) 2 2 2 n/a

η3 (poise) 2 2 2 2

η4 (poise) n/a 50 50 50

Case 1 - Rectangular

VF convergence (cm) x01 = 0.03 x01 = 0.03 x01 = 0.03 x01 = 0.03
x02 = 0.03 x02 = 0.03 x02 = 0.03 x02 = 0.03

VF bulging (cm) 0 0 0 0

Case 2 - 1X convergent

VF convergence (cm) x01 = 0.06 x01 = 0.06 x01 = 0.06 x01 = 0.06
x02 = 0.03 x02 = 0.03 x02 = 0.03 x02 = 0.03

VF bulging (cm) 0 0 0 0

Case 3 - 2X convergent

VF convergence (cm) x01 = 0.12 x01 = 0.12 x01 = 0.12 x01 = 0.12
x02 = 0.03 x02 = 0.03 x02 = 0.03 x02 = 0.03

VF bulging (cm) 0 0 0 0

Case 4 - 1X convergent with bulging

VF convergence (cm) x01 = 0.06 x01 = 0.06 x01 = 0.06 x01 = 0.06
x02 = 0.03 x02 = 0.03 x02 = 0.03 x02 = 0.03

VF bulging (cm) 0.03 0.03 0.03 0.03

Case 5 – 2X convergent with bulging

VF convergence (cm) x01 = 0.12 x01 = 0.12 x01 = 0.12 x01 = 0.12
x02 = 0.03 x02 = 0.03 x02 = 0.03 x02 = 0.03

VF bulging (cm) 0.07 0.07 0.07 0.07