Coverage for qpdk / models / capacitor.py: 100%
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« prev ^ index » next coverage.py v7.13.4, created at 2026-03-14 10:27 +0000
1"""Capacitor Models."""
3from functools import partial
5import jax
6import jax.numpy as jnp
7import sax
8from gdsfactory.typings import CrossSectionSpec
10from qpdk.models.constants import DEFAULT_FREQUENCY, ε_0
11from qpdk.models.cpw import cpw_ep_r_from_cross_section, cpw_z0_from_cross_section
12from qpdk.models.generic import capacitor
13from qpdk.models.math import (
14 capacitance_per_length_conformal,
15 ellipk_ratio,
16 epsilon_eff,
17)
20@partial(jax.jit, inline=True)
21def plate_capacitor_capacitance_analytical(
22 length: float,
23 width: float,
24 gap: float,
25 ep_r: float,
26) -> float:
27 r"""Analytical formula for plate capacitor capacitance.
29 The model assumes two coplanar rectangular pads on a substrate.
30 The capacitance is calculated using conformal mapping:
32 .. math::
34 k &= \frac{s}{s + 2W} \\
35 k' &= \sqrt{1 - k^2} \\
36 \epsilon_{\text{eff}} &= \frac{\epsilon_r + 1}{2} \\
37 C &= \epsilon_0 \epsilon_{\text{eff}} L \frac{K(k')}{K(k)}
39 where :math:`s` is the gap, :math:`W` is the pad width, and :math:`L` is the pad length.
41 See :cite:`chenCompactInductorcapacitorResonators2023`.
42 """
43 # Conformal mapping for coplanar pads
44 k_sq = (gap / (gap + 2 * width)) ** 2
46 # C = ε_0 * ε_eff * L * K(k') / K(k)
47 # Uses K(1-m)/K(m) which is the inverse of ellipk_ratio(m)
48 c_pul = ε_0 * epsilon_eff(ep_r) / ellipk_ratio(k_sq)
50 return (length * 1e-6) * c_pul
53@partial(jax.jit, inline=True)
54def interdigital_capacitor_capacitance_analytical(
55 fingers: int,
56 finger_length: float,
57 finger_gap: float,
58 thickness: float,
59 ep_r: float,
60) -> jax.Array:
61 r"""Analytical formula for interdigital capacitor capacitance.
63 The formula uses conformal mapping for the interior and exterior regions of
64 the interdigital structure:
66 .. math::
68 \eta &= \frac{w}{w + g} \\
69 k_i &= \sin\left(\frac{\pi \eta}{2}\right) \\
70 k_e &= \frac{2\sqrt{\eta}}{1 + \eta} \\
71 C_i &= \epsilon_0 L (\epsilon_r + 1) \frac{K(k_i)}{K(k_i')} \\
72 C_e &= \epsilon_0 L (\epsilon_r + 1) \frac{K(k_e)}{K(k_e')}
74 The total mutual capacitance for :math:`n` fingers is:
76 .. math::
78 C = \begin{cases}
79 C_e / 2 & \text{if } n=2 \\
80 (n - 3) \frac{C_i}{2} + 2 \frac{C_i C_e}{C_i + C_e} & \text{if } n > 2
81 \end{cases}
83 where :math:`w` is the finger thickness (width), :math:`g` is the finger gap, and
84 :math:`L` is the overlap length.
86 See :cite:`igrejaAnalyticalEvaluationInterdigital2004,gonzalezDesignFabricationInterdigital2015`.
87 """
88 # Geometric parameters
89 n = fingers
90 l_overlap = finger_length * 1e-6 # Overlap length in m
91 w = thickness # Finger width
92 g = finger_gap # Finger gap
93 η = w / (w + g) # Metallization ratio
95 # Elliptic integral moduli squared
96 ki_sq = jnp.sin(jnp.pi * η / 2) ** 2
97 ke_sq = (2 * jnp.sqrt(η) / (1 + η)) ** 2
99 # Capacitances per unit length (interior and exterior)
100 # Factor is 2.0 since interdigital formula uses (ep_r + 1) = 2 * ep_eff
101 c_i = l_overlap * 2.0 * capacitance_per_length_conformal(m=ki_sq, ep_r=ep_r)
102 c_e = l_overlap * 2.0 * capacitance_per_length_conformal(m=ke_sq, ep_r=ep_r)
104 # Total mutual capacitance
105 # Simplifies to c_e/2 for n=2
106 return jnp.where( # pyrefly: ignore[bad-return]
107 n == 2,
108 c_e / 2,
109 (n - 3) * c_i / 2 + 2 * (c_i * c_e) / (c_i + c_e),
110 )
113def plate_capacitor(
114 *,
115 f: sax.FloatArrayLike = DEFAULT_FREQUENCY,
116 length: float = 26.0,
117 width: float = 5.0,
118 gap: float = 7.0,
119 cross_section: CrossSectionSpec = "cpw",
120) -> sax.SDict:
121 r"""Plate capacitor Sax model.
123 Args:
124 f: Array of frequency points in Hz
125 length: Length of the capacitor pad in μm
126 width: Width of the capacitor pad in μm
127 gap: Gap between plates in μm
128 cross_section: Cross-section specification
130 Returns:
131 sax.SDict: S-parameters dictionary
132 """
133 f_arr = jnp.asarray(f)
134 z0 = cpw_z0_from_cross_section(cross_section, f_arr)
135 ep_r = cpw_ep_r_from_cross_section(cross_section)
136 capacitance = plate_capacitor_capacitance_analytical(
137 length=length, width=width, gap=gap, ep_r=ep_r
138 )
139 return capacitor(f=f_arr, capacitance=capacitance, z0=z0)
142def interdigital_capacitor(
143 *,
144 f: sax.FloatArrayLike = DEFAULT_FREQUENCY,
145 fingers: int = 4,
146 finger_length: float = 20.0,
147 finger_gap: float = 2.0,
148 thickness: float = 5.0,
149 cross_section: CrossSectionSpec = "cpw",
150) -> sax.SDict:
151 r"""Interdigital capacitor Sax model.
153 Args:
154 f: Array of frequency points in Hz
155 fingers: Total number of fingers (must be >= 2)
156 finger_length: Length of each finger in μm
157 finger_gap: Gap between adjacent fingers in μm
158 thickness: Thickness of fingers in μm
159 cross_section: Cross-section specification
161 Returns:
162 sax.SDict: S-parameters dictionary
163 """
164 f_arr = jnp.asarray(f)
165 z0 = cpw_z0_from_cross_section(cross_section, f_arr)
166 ep_r = cpw_ep_r_from_cross_section(cross_section)
167 capacitance = interdigital_capacitor_capacitance_analytical(
168 fingers=fingers,
169 finger_length=finger_length,
170 finger_gap=finger_gap,
171 thickness=thickness,
172 ep_r=ep_r,
173 )
174 return capacitor(f=f_arr, capacitance=capacitance, z0=z0)
177if __name__ == "__main__":
178 import matplotlib.pyplot as plt
180 # 1. Plot Plate Capacitor Capacitance vs. Length for different Gaps
181 lengths = jnp.linspace(10, 500, 100)
182 gaps_plate = jnp.geomspace(1.0, 20.0, 5)
183 width_plate = 10.0
184 ep_r = 11.7
186 plt.figure(figsize=(10, 6))
188 # Broadcast to compute total capacitance for all lengths and gaps (shape: (5, 100))
189 # length * 1e-6 happens in the analytical formula, here we replicate it
190 capacitances_plate = (
191 plate_capacitor_capacitance_analytical(
192 length=lengths[None, :],
193 width=width_plate,
194 gap=gaps_plate[:, None],
195 ep_r=ep_r,
196 )
197 * 1e15
198 ) # Convert to fF
200 for i, gap in enumerate(gaps_plate):
201 plt.plot(lengths, capacitances_plate[i], label=f"gap = {gap:.1f} µm")
203 plt.xlabel("Pad Length (µm)")
204 plt.ylabel("Capacitance (fF)")
205 plt.title(
206 rf"Plate Capacitor Capacitance ($\mathtt{{width}}=${width_plate} µm, $\epsilon_r={ep_r}$)"
207 )
208 plt.grid(True)
209 plt.legend()
210 plt.tight_layout()
211 plt.show()
213 # 2. Plot Interdigital Capacitor Capacitance vs. Finger Length for different Finger Counts
214 finger_lengths = jnp.linspace(10, 100, 100)
215 finger_counts = jnp.arange(2, 11, 2) # [2, 4, 6, 8, 10]
216 finger_gap = 2.0
217 thickness = 5.0
219 plt.figure(figsize=(10, 6))
221 # Broadcast to compute total capacitance for all lengths and counts (shape: (5, 100))
222 capacitances_idc = (
223 interdigital_capacitor_capacitance_analytical(
224 fingers=finger_counts[:, None],
225 finger_length=finger_lengths[None, :],
226 finger_gap=finger_gap,
227 thickness=thickness,
228 ep_r=ep_r,
229 )
230 * 1e15
231 ) # Convert to fF
233 for i, n in enumerate(finger_counts):
234 plt.plot(finger_lengths, capacitances_idc[i], label=f"n = {n} fingers")
236 plt.xlabel("Overlap Length (µm)")
237 plt.ylabel("Mutual Capacitance (fF)")
238 plt.title(
239 rf"Interdigital Capacitor Capacitance ($\mathtt{{finger\_gap}}=${finger_gap} µm, $\mathtt{{thickness}}=${thickness} µm, $\epsilon_r={ep_r}$)"
240 )
241 plt.grid(True)
242 plt.legend()
243 plt.tight_layout()
244 plt.show()