Level 1 — RecognitionGuidance, Navigation & Control (GNC)

Guidance, Navigation & Control (GNC)

20 minutes40 marksprintable — key stays hidden on paper

Chapter: 3.5 Guidance, Navigation & Control Level: 1 — Recognition (MCQ, matching, true/false with justification) Time limit: 20 minutes Total marks: 40


Section A — Multiple Choice (1 mark each; 16 marks)

Choose the single best answer.

Q1. An accelerometer in free-fall (no thrust, only gravity) measures a specific force of:

  • (a) gg downward
  • (b) gg upward
  • (c) zero
  • (d) 2g2g

Q2. The 3-2-1 Euler angle sequence rotates by angles in the order:

  • (a) roll, pitch, yaw
  • (b) yaw, pitch, roll
  • (c) pitch, yaw, roll
  • (d) yaw, roll, pitch

Q3. The unit quaternion constraint is:

  • (a) q0+q1+q2+q3=1q_0 + q_1 + q_2 + q_3 = 1
  • (b) q02+q12+q22+q32=1q_0^2 + q_1^2 + q_2^2 + q_3^2 = 1
  • (c) q02q12q22q32=1q_0^2 - q_1^2 - q_2^2 - q_3^2 = 1
  • (d) q12+q22+q32=1q_1^2 + q_2^2 + q_3^2 = 1

Q4. Gimbal lock in a 3-2-1 Euler sequence occurs at pitch angle:

  • (a) θ=0\theta = 0
  • (b) θ=45\theta = 45^\circ
  • (c) θ=±90\theta = \pm 90^\circ
  • (d) θ=180\theta = 180^\circ

Q5. The DCM kinematics equation is:

  • (a) C˙=[ω×]C\dot{C} = [\omega\times]C
  • (b) C˙=[ω×]C\dot{C} = -[\omega\times]C
  • (c) C˙=C[ω×]\dot{C} = C[\omega\times]
  • (d) C˙=CT[ω×]\dot{C} = -C^T[\omega\times]

Q6. A continuous-time linear system x˙=Ax\dot{x}=Ax is asymptotically stable if and only if:

  • (a) all eigenvalues of AA have positive real part
  • (b) all eigenvalues of AA have negative real part
  • (c) AA is symmetric
  • (d) det(A)=0\det(A)=0

Q7. Proportional navigation guidance commands acceleration proportional to:

  • (a) range to target
  • (b) NVcλ˙N\,V_c\,\dot\lambda (LOS rotation rate)
  • (c) closing velocity only
  • (d) the target's absolute acceleration

Q8. The Kalman gain is chosen to:

  • (a) maximize the trace of the covariance
  • (b) minimize the trace of the posterior error covariance
  • (c) make the innovation zero
  • (d) set the process noise to zero

Q9. A PID controller output is:

  • (a) Kpe+Kiedt+Kde˙K_p e + K_i \int e\,dt + K_d \dot{e}
  • (b) Kpe+Kie˙+KdedtK_p e + K_i \dot{e} + K_d \int e\,dt
  • (c) KpedtK_p \int e\,dt
  • (d) Kpe˙K_p \dot{e}

Q10. The controllability matrix for (A,B)(A,B) with ARn×nA\in\mathbb{R}^{n\times n} is:

  • (a) [C CA  CAn1]T[C\ CA\ \cdots\ CA^{n-1}]^T
  • (b) [B AB A2B  An1B][B\ AB\ A^2B\ \cdots\ A^{n-1}B]
  • (c) [A B][A\ B]
  • (d) A1BA^{-1}B

Q11. Gyroscope measurement error typically includes:

  • (a) bias and noise
  • (b) only quantization
  • (c) gravity coupling only
  • (d) no error (ideal)

Q12. GPS position is found from at least how many satellite pseudoranges (for 3D + clock)?

  • (a) 2
  • (b) 3
  • (c) 4
  • (d) 6

Q13. In the Nyquist stability criterion, stability is assessed by counting encirclements of the point:

  • (a) 00
  • (b) +1+1
  • (c) 1-1
  • (d) ++\infty

Q14. The LQR optimal gain requires solving the:

  • (a) Lyapunov equation
  • (b) algebraic Riccati equation
  • (c) Bellman ODE only
  • (d) characteristic polynomial of BB

Q15. Modified Rodrigues parameters are attractive because they are:

  • (a) always exactly the Euler angles
  • (b) compact and singularity-free over a large range
  • (c) a 4-parameter set with a constraint
  • (d) only defined for small rotations

Q16. A control moment gyroscope (CMG) provides high torque but suffers from:

  • (a) zero-crossing friction
  • (b) gimbal singularities
  • (c) plume impingement
  • (d) pseudorange bias

Section B — Matching (1 mark each; 12 marks)

Match each item in Column X to the correct description in Column Y. Write pairs (e.g., M1–?).

Column X Column Y
M1. Complementary filter A. Two vector measurements → attitude
M2. TRIAD method B. Optimal linear estimator, predict/update
M3. Kalman filter C. Simple frequency-domain sensor blend
M4. EKF D. Sigma points, no Jacobians
M5. UKF E. Linearization via Jacobians
M6. IMU F. Accelerometer + gyroscope package
Column X Column Y
M7. Root locus P. Magnitude & phase vs frequency
M8. Bode plot Q. Poles migrate as gain varies
M9. Observability matrix R. Distributes torque among thrusters/wheels
M10. Pole placement S. Ackermann's formula
M11. RCS thruster selection T. Stack of C,CA,,CAn1C, CA, \dots, CA^{n-1}
M12. Reaction wheel U. Momentum storage, zero-crossing issue

Section C — True/False WITH one-line justification (2 marks each: 1 T/F + 1 justification; 12 marks)

Q17. "Quaternions avoid gimbal lock entirely." — True/False? Justify.

Q18. "The gravity vector coincides with the specific force measured by an accelerometer on a table." — True/False? Justify.

Q19. "Adding more, well-spread GPS satellites reduces the geometric dilution of precision (GDOP)." — True/False? Justify.

Q20. "A system can be stabilized by full-state feedback pole placement only if it is controllable." — True/False? Justify.

Q21. "In a 3-2-1 DCM, the total rotation matrix is R1(ϕ)R2(θ)R3(ψ)R_1(\phi)R_2(\theta)R_3(\psi) applied to a vector expressed in inertial frame to get body frame." — True/False? Justify.

Q22. "The LQG controller can be designed by separately designing the LQR and the Kalman filter (separation principle)." — True/False? Justify.

Answer keyMark scheme & solutions

Section A (1 mark each)

Q1 — (c) zero. In free-fall, the only force is gravity; an accelerometer measures non-gravitational specific force f=agf = a - g. In free-fall a=ga=g, so f=0f=0. (This is why accelerometers can't sense gravity directly.)

Q2 — (b) yaw, pitch, roll. The "3-2-1" refers to rotation axes in order: 3rd axis (yaw ψ), then 2nd (pitch θ), then 1st (roll φ).

Q3 — (b) q02+q12+q22+q32=1q_0^2+q_1^2+q_2^2+q_3^2=1. A unit quaternion has norm 1 to represent a pure rotation.

Q4 — (c) θ=±90\theta=\pm90^\circ. At pitch =±90=\pm90^\circ the roll and yaw axes align → one DOF lost → gimbal lock.

Q5 — (b) C˙=[ω×]C\dot{C}=-[\omega\times]C. Standard body-to-inertial DCM kinematics with body rates.

Q6 — (b) negative real parts. Hurwitz condition: all eigenvalues in open left half-plane ⇒ modes eλt0e^{\lambda t}\to 0.

Q7 — (b) NVcλ˙N V_c \dot\lambda. PN commands lateral acceleration proportional to closing velocity times line-of-sight rate.

Q8 — (b) minimize trace of posterior covariance. Kalman gain minimizes expected squared error = trace of P+P^+.

Q9 — (a) Kpe+Kiedt+Kde˙K_p e + K_i\int e\,dt + K_d\dot e. Definition of PID.

Q10 — (b) [B AB  An1B][B\ AB\ \dots\ A^{n-1}B]. Controllability matrix; full rank nn ⇒ controllable.

Q11 — (a) bias and noise. Gyro model: ω~=ω+b+n\tilde\omega = \omega + b + n.

Q12 — (c) 4. Three coordinates plus receiver clock bias = 4 unknowns → 4 pseudoranges.

Q13 — (c) 1-1. Nyquist counts encirclements of 1+j0-1+j0.

Q14 — (b) algebraic Riccati equation. K=R1BTPK=R^{-1}B^TP, with PP from the ARE.

Q15 — (b) compact and singularity-free over a large range. MRPs are a 3-parameter set with singularity only at 360360^\circ.

Q16 — (b) gimbal singularities. CMGs give high torque amplification but can hit singular gimbal configurations.

Section B (1 mark each)

M1–C, M2–A, M3–B, M4–E, M5–D, M6–F, M7–Q, M8–P, M9–T, M10–S, M11–R, M12–U.

Rationale: complementary filter = simple frequency blend; TRIAD uses two vectors; KF is optimal predict/update; EKF linearizes (Jacobians); UKF uses sigma points; IMU = accel+gyro; root locus tracks poles vs gain; Bode = magnitude/phase; observability matrix stacks C,CA,C, CA,\dots; pole placement via Ackermann; RCS selection distributes torque; reaction wheels store momentum with zero-crossing friction.

Section C (1 mark T/F + 1 mark justification)

Q17 — TRUE. Quaternions have no coordinate singularity; the 4-parameter representation with unit constraint parametrizes SO(3) globally (double cover), so no gimbal lock.

Q18 — FALSE. On a table a=0a=0, so specific force f=gf=-g (points opposite gravity, magnitude gg upward as reaction). The accelerometer reads the support force, not the gravity vector's direction—so it is anti-parallel to gg, not coincident.

Q19 — TRUE. More, geometrically well-distributed satellites make the geometry matrix better conditioned, lowering GDOP (better dilution). (Poorly spread satellites still give high GDOP.)

Q20 — TRUE. Arbitrary pole placement via state feedback is possible iff (A,B)(A,B) is controllable; controllability is the condition for full eigenvalue assignment. (Stabilizability suffices if uncontrollable modes are already stable, but full placement needs controllability.)

Q21 — TRUE. The 3-2-1 DCM from inertial to body is Cbi1=R1(ϕ)R2(θ)R3(ψ)C_b^i{}^{-1}=R_1(\phi)R_2(\theta)R_3(\psi); applied to an inertial vector it yields body-frame components. (Order of matrix multiplication = reverse order of physical rotation, consistent with 3-2-1.)

Q22 — TRUE. The separation principle guarantees LQR (state feedback) and Kalman filter (estimator) can be designed independently; combined LQG is optimal and the closed-loop eigenvalues are the union of both designs.

[
  {"claim":"Free-fall specific force is zero: f = a - g with a=g",
   "code":"a=g=9.81; f=a-g; result=(f==0)"},
  {"claim":"Unit quaternion norm-squared equals 1",
   "code":"q0,q1,q2,q3=Rational(1,2),Rational(1,2),Rational(1,2),Rational(1,2); result=(q0**2+q1**2+q2**2+q3**2==1)"},
  {"claim":"GPS 3D+clock requires 4 unknowns hence 4 satellites",
   "code":"unknowns=3+1; result=(unknowns==4)"},
  {"claim":"Hurwitz: eigenvalues of stable A=[[0,1],[-2,-3]] have negative real parts",
   "code":"A=Matrix([[0,1],[-2,-3]]); ev=list(A.eigenvals().keys()); result=all(re(e)<0 for e in ev)"},
  {"claim":"Controllability matrix of A=[[0,1],[0,0]],B=[[0],[1]] has full rank 2",
   "code":"A=Matrix([[0,1],[0,0]]); B=Matrix([[0],[1]]); Cm=B.row_join(A*B); result=(Cm.rank()==2)"}
]