Cosplay/nhf/geometry.py

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"""
Geometry functions
"""
from typing import Tuple, Optional
import math
def min_radius_contraction_span_pos(
d_open: float,
d_closed: float,
theta: float,
) -> Tuple[float, float]:
"""
Calculates the position of the two ends of an actuator, whose fully opened
length is `d_open`, closed length is `d_closed`, and whose motion spans a
range `theta` (in radians). Returns (r, phi): If one end of the actuator is
held at `(r, 0)`, then the other end will trace an arc `r` away from the
origin with span `theta`
Let `P` (resp. `P'`) be the position of the front of the actuator when its
fully open (resp. closed), `Q` be the position of the back of the actuator,
we note that `OP = OP' = OQ`.
"""
assert d_open > d_closed
assert 0 < theta < math.pi
pq2 = d_open * d_open
p_q2 = d_closed * d_closed
# angle of PQP'
psi = 0.5 * theta
# |P-P'|, via the triangle PQP'
pp_2 = pq2 + p_q2 - 2 * d_open * d_closed * math.cos(psi)
r2 = pp_2 / (2 - 2 * math.cos(theta))
# Law of cosines on POQ:
phi = math.acos(1 - pq2 / 2 / r2)
return math.sqrt(r2), phi
def min_tangent_contraction_span_pos(
d_open: float,
d_closed: float,
theta: float,
) -> Tuple[float, float, float]:
"""
Returns `(r, phi, r')` where `r` is the distance of the arm to origin, `r'`
is the distance of the base to origin, and `phi` the angle in the open
state.
"""
assert d_open > d_closed
assert 0 < theta < math.pi
# Angle of OPQ = OPP'
pp_ = d_open - d_closed
pq = d_open
p_q = d_closed
a = (math.pi - theta) / 2
# Law of sines on POP'
r = math.sin(a) / math.sin(theta) * pp_
# Law of cosine on OPQ
oq = math.sqrt(r * r + pq * pq - 2 * r * pq * math.cos(a))
# Law of sines on OP'Q. Not using OPQ for numerical reasons since the angle
# `phi` could be very close to `pi/2`
phi_ = math.asin(math.sin(a) / oq * p_q)
phi = phi_ + theta
assert theta <= phi < math.pi
return r, phi, oq
def contraction_span_pos_from_radius(
d_open: float,
d_closed: float,
theta: float,
r: Optional[float] = None,
smaller: bool = True,
) -> Tuple[float, float, float]:
"""
Returns `(r, phi, r')`
Set `smaller` to false to use the other solution, which has a larger
profile.
"""
if r is None:
return min_tangent_contraction_span_pos(
d_open=d_open,
d_closed=d_closed,
theta=theta)
assert 0 < theta < math.pi
assert d_open > d_closed
assert r > 0
# Law of cosines
pp_ = r * math.sqrt(2 * (1 - math.cos(theta)))
d = d_open - d_closed
assert pp_ > d, f"Triangle inequality is violated. This joint is impossible: {pp_}, {d}"
assert d_open + d_closed > pp_, f"The span is too great to cover with this stroke length: {pp_}"
# Angle of PP'Q, via a numerically stable acos
beta = math.acos(
- d / pp_ * (1 + d / (2 * d_closed))
+ pp_ / (2 * d_closed))
# Two solutions based on angle complementarity
if smaller:
contra_phi = beta - (math.pi - theta) / 2
else:
# technically there's a 2pi in front
contra_phi = -(math.pi - theta) / 2 - beta
# Law of cosines, calculates `r'`
r_ = math.sqrt(
r * r + d_closed * d_closed - 2 * r * d_closed * math.cos(contra_phi)
)
# sin phi_ / P'Q = sin contra_phi / r'
phi_ = math.asin(math.sin(contra_phi) / r_ * d_closed)
assert phi_ > 0, f"Actuator would need to traverse pass its minimal point, {math.degrees(phi_)}"
assert 0 <= theta + phi_ <= math.pi
return r, theta + phi_, r_