Statics and Dynamics Quiz: Checking Solutions
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Checking SolutionsQuestion 1 of 7

A student solves for the angular velocity ω\omega of a uniform disk (mass mm, radius RR) rolling without slipping down an inclined plane of angle θ\theta after its center has traveled a distance dd along the incline, starting from rest. The student reports: ω=4gdsinθ3R2\omega = \sqrt{\frac{4gd\sin\theta}{3R^2}}

The student performs a unit check and confirms the expression has units of rad/s. Which of the following most completely and correctly evaluates whether the formula should be accepted?

The formula should be rejected. Although the unit check passes, the coefficient 4/34/3 violates the physical constraint that all energy-method coefficients for rolling bodies must be rational numbers strictly less than 1, since the rolling kinetic energy is always a fraction of the total kinetic energy. This indicates an error in the moment-of-inertia calculation for the disk.
The formula should be accepted with caution. The unit check passes, and the limiting cases θ0\theta \to 0 and d0d \to 0 both correctly give ω0\omega \to 0. These checks are consistent with the formula, but they cannot validate the coefficient 4/34/3 — an incorrect coefficient such as 11 or 22 would pass the same limiting-case tests. Independent verification via energy methods confirms the coefficient is correct, but that requires re-deriving the result.
The formula should be rejected because the limiting case θ90\theta \to 90^\circ yields ω=4gd/(3R2)\omega = \sqrt{4gd/(3R^2)}, but rolling without slipping on a vertical surface is physically impossible since there is no normal force to generate the required friction. A valid formula must give an undefined or zero result at this limit, so the formula's finite prediction reveals a fundamental modeling error.
The formula should be rejected on dimensional grounds. Applying the no-slip constraint vc=ωRv_c = \omega R requires that ω\omega scale as R1R^{-1}, but inspection of the formula shows it scales as R1R^{-1} only if dd is independent of RR. Since the problem does not specify this independence, the formula conflates geometric and kinematic variables and cannot be accepted without additional clarification.
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Statics and Dynamics Quiz

Statics and Dynamics Quiz: Checking Solutions

Practice Checking Solutions in Statics and Dynamics with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

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This quiz focuses on Checking Solutions, giving you a quick way to practice the rules, question types, and explanations that matter most for Statics and Dynamics.

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Question 1

A student solves for the angular velocity ω\omega of a uniform disk (mass mm, radius RR) rolling without slipping down an inclined plane of angle θ\theta after its center has traveled a distance dd along the incline, starting from rest. The student reports: ω=4gdsinθ3R2\omega = \sqrt{\frac{4gd\sin\theta}{3R^2}}

The student performs a unit check and confirms the expression has units of rad/s. Which of the following most completely and correctly evaluates whether the formula should be accepted?

  1. The formula should be rejected. Although the unit check passes, the coefficient 4/34/3 violates the physical constraint that all energy-method coefficients for rolling bodies must be rational numbers strictly less than 1, since the rolling kinetic energy is always a fraction of the total kinetic energy. This indicates an error in the moment-of-inertia calculation for the disk.
  2. The formula should be accepted with caution. The unit check passes, and the limiting cases θ0\theta \to 0 and d0d \to 0 both correctly give ω0\omega \to 0. These checks are consistent with the formula, but they cannot validate the coefficient 4/34/3 — an incorrect coefficient such as 11 or 22 would pass the same limiting-case tests. Independent verification via energy methods confirms the coefficient is correct, but that requires re-deriving the result. (correct answer)
  3. The formula should be rejected because the limiting case θ90\theta \to 90^\circ yields ω=4gd/(3R2)\omega = \sqrt{4gd/(3R^2)}, but rolling without slipping on a vertical surface is physically impossible since there is no normal force to generate the required friction. A valid formula must give an undefined or zero result at this limit, so the formula's finite prediction reveals a fundamental modeling error.
  4. The formula should be rejected on dimensional grounds. Applying the no-slip constraint vc=ωRv_c = \omega R requires that ω\omega scale as R1R^{-1}, but inspection of the formula shows it scales as R1R^{-1} only if dd is independent of RR. Since the problem does not specify this independence, the formula conflates geometric and kinematic variables and cannot be accepted without additional clarification.
Explanation: When evaluating a physics formula, you should think in layers: dimensional analysis first, then limiting cases, then coefficient verification. Passing one layer doesn't mean passing all of them — and understanding what each layer can and cannot tell you is exactly what this question tests. The formula ω=4gdsinθ3R2\omega = \sqrt{\frac{4gd\sin\theta}{3R^2}} can be verified by energy conservation. Setting potential energy loss equal to total kinetic energy (translational plus rotational, using I=12mR2I = \frac{1}{2}mR^2 for a disk and the no-slip condition vc=ωRv_c = \omega R) yields exactly this expression with coefficient 4/34/3. So the formula is correct. Choice B is right because it honestly acknowledges what the checks do and don't prove: the unit check and limiting cases (θ0\theta \to 0, d0d \to 0 both giving ω0\omega \to 0) are consistent with the formula but cannot distinguish the correct coefficient from an incorrect one like 11 or 22. Full confidence requires re-deriving the result independently. Choice A is wrong because it invents a false rule. The coefficient 4/34/3 appears in the denominator under the radical when you work through the energy algebra correctly — there is no requirement that such coefficients be less than 1. Choice C is wrong because it misinterprets what a formula's domain of validity means. The formula models rolling without slipping; applying it at θ=90°\theta = 90° gives a mathematically finite answer, but the physical model simply breaks down there. That's a modeling limitation, not a derivation error — the formula isn't required to self-destruct at its boundary. Choice D introduces a false dimensional conflict. The variable dd is an independent displacement along the incline, not a function of RR, so there is no conflation of variables. Strategy tip: On problems asking you to evaluate a formula, always ask: "What can this test actually detect, and what can it miss?" Limiting cases and unit checks are necessary but not sufficient — they can never validate a specific numerical coefficient.

Question 2

A student analyzes a pin-connected truss and, using the method of joints, reports that member AB carries a force of FAB=85 kNF_{AB} = 85\text{ kN} in tension. As a check, the student notes: (1) all external loads are in kN, (2) the geometry is dimensionally consistent, and (3) the force is positive, confirming the assumed tension direction.

A more experienced engineer reviews the solution and argues that the student's three checks are necessary but not sufficient, and identifies a fourth check that could reveal an error the student missed. Which of the following is the most rigorous additional check available without re-solving the entire problem?

  1. Verify that FAB=85 kNF_{AB} = 85\text{ kN} does not exceed the allowable tensile capacity of the member's cross-section. A force exceeding the material strength would be physically unreasonable for a stable structure, indicating that an error was made somewhere in the equilibrium analysis.
  2. Apply the method of sections by cutting through member AB and two other members, then write equilibrium equations for the resulting free body. Agreement with 85 kN in tension corroborates the result using an independent equation set; a disagreement reveals a computational error that the three original checks could not detect. (correct answer)
  3. Confirm that the sum of all reported member forces in the truss equals zero, since global force balance requires tensile and compressive member forces to cancel when summed across all members, providing a system-level consistency check that is independent of the method of joints.
  4. Apply Maxwell's reciprocal theorem, which relates member forces under reciprocal unit loads, to verify that the force in AB due to the applied loading equals the force predicted by reciprocal loading at joint B — providing an independent analytical cross-check of the reported 85 kN value.
Explanation: Whenever you encounter a question about verifying structural analysis results, ask yourself: does this check use a truly independent method, or does it just repackage the same assumptions? The method of joints produces equilibrium equations at each joint individually. Its weakness is that a computational error at one joint can propagate invisibly through the solution — and the three checks the student performed (unit consistency, sign convention, dimensional geometry) all operate within that same framework. None of them catch arithmetic mistakes or incorrect force directions in the equilibrium equations themselves. The method of sections, choice B, is the correct answer because it constructs an entirely separate free-body diagram by cutting through the truss — including member AB — and writes independent equilibrium equations for that cut section. If this independent calculation also yields FAB=85 kNF_{AB} = 85\text{ kN} in tension, you have genuine corroboration. If it disagrees, you've detected an error that no internal consistency check could have found. This is what makes it rigorous: it's a mathematically independent verification. Choice A is a material strength check, not a mechanics verification. Whether 85 kN exceeds a cross-section's capacity tells you nothing about whether the equilibrium analysis was performed correctly — it's a design consideration, not a structural analysis check. Choice C is based on a false premise. Member forces in a truss do not sum to zero globally; that statement confuses internal forces with external reactions. This "check" would never reveal a real error. Choice D misapplies Maxwell's reciprocal theorem, which relates displacements under reciprocal loads, not directly member forces under a specific loading case. It cannot straightforwardly verify a single member force value. Study tip: On statics questions asking for "independent verification," always favor methods that use a completely different free-body diagram and equation set — that's the gold standard for catching computational errors.

Question 3

A student applies the work-energy theorem to a system and derives the final speed of a block after it slides a distance dd down a rough incline of angle θ\theta, starting from rest, as: v=2gd(sinθ+μkcosθ)v = \sqrt{2gd(\sin\theta + \mu_k\cos\theta)} The student performs a unit check and confirms the expression has units of m/s. Which of the following best identifies whether this answer should be accepted or rejected, and why?

  1. The answer should be rejected, but only for angles where μkcosθ>sinθ\mu_k\cos\theta > \sin\theta, because in that case the expression under the radical becomes larger than 2gdsinθ2gd\sin\theta, yielding a speed greater than the frictionless result — a physically impossible outcome that proves the sign is wrong for those specific angles.
  2. The answer should be accepted. The unit check confirms dimensional consistency, and the presence of both sinθ\sin\theta and cosθ\cos\theta terms is structurally correct since both the gravitational component and the normal force (which drives friction) depend on the angle; the sign of the friction term cannot be determined without knowing the direction convention.
  3. The answer should be rejected. The friction force opposes motion, so kinetic friction removes energy from the system; the work done by friction is negative. The correct expression is v=2gd(sinθμkcosθ)v = \sqrt{2gd(\sin\theta - \mu_k\cos\theta)}. The plus sign inside the radical causes the formula to predict a speed greater than the frictionless case, which violates physical reasonableness — friction cannot accelerate the block. (correct answer)
  4. The answer should be accepted for θ>45\theta > 45^\circ because at steep angles sinθ>cosθ\sin\theta > \cos\theta, making the gravitational term dominant and rendering the sign of the friction term physically irrelevant to the reasonableness check.
Explanation: Whenever you apply the work-energy theorem on an incline, your first instinct after getting an answer should be a physical reasonableness check, not just a unit check. Ask yourself: does this result make sense compared to a simpler, known case? Here, the frictionless result is v=2gdsinθv = \sqrt{2gd\sin\theta}. Friction opposes motion — it removes mechanical energy from the system, so the block must arrive at the bottom slower than the frictionless case. The work done by kinetic friction is negative: Wf=μkmgcosθdW_f = -\mu_k mg\cos\theta \cdot d. Applying the work-energy theorem correctly gives 12mv2=mgdsinθμkmgdcosθ\frac{1}{2}mv^2 = mgd\sin\theta - \mu_k mgd\cos\theta, yielding v=2gd(sinθμkcosθ)v = \sqrt{2gd(\sin\theta - \mu_k\cos\theta)}. The student's plus sign instead produces a speed larger than the frictionless result — friction is effectively accelerating the block, which is physically impossible. C correctly identifies both the sign error and the physical violation, making it the right choice. A is wrong because it mischaracterizes the problem. The formula is incorrect at all angles, not just where μkcosθ>sinθ\mu_k\cos\theta > \sin\theta; the flaw is the wrong sign, period. Pointing to a subset of angles doesn't identify the root error. B is wrong because it treats a passing unit check as sufficient validation. Units confirm dimensional consistency, but they cannot detect sign errors — a formula and its negative can have identical units. D is wrong because physical laws don't become "irrelevant" at steep angles. A sign error is a sign error regardless of which term dominates numerically. Strategy tip: Always benchmark your answer against a simpler limiting case. If removing friction makes the result slower than your derived formula, your signs are wrong — no unit check will catch that.

Question 4

A student solves for the magnitude of the resultant of two concurrent forces F1=50 NF_1 = 50\text{ N} and F2=120 NF_2 = 120\text{ N} acting at an angle α\alpha to each other, obtaining R=140 NR = 140\text{ N}. As a check, the student notes that when α=0\alpha = 0^\circ the formula gives R=170 NR = 170\text{ N}, and when α=180\alpha = 180^\circ it gives R=70 NR = 70\text{ N}. Which statement about the original answer is most justified by these limiting-case checks?

  1. The answer is plausible: R=140 NR = 140\text{ N} lies strictly between the minimum of 70 N (forces opposing) and maximum of 170 N (forces aligned), which is a necessary condition for any valid resultant at an intermediate angle. (correct answer)
  2. The answer must be correct: passing both the α=0\alpha = 0^\circ and α=180\alpha = 180^\circ limiting cases is sufficient to confirm that the formula and the specific numerical result are free of errors.
  3. The answer is suspicious: for α=90\alpha = 90^\circ the resultant should be 502+1202=130 N\sqrt{50^2 + 120^2} = 130\text{ N}, and since 140 N > 130 N, the forces must be acting at an angle less than 90°. Because the problem does not specify α\alpha, the result 140 N is outside the acceptable range and should be rejected.
  4. The answer is suspicious: the triangle inequality requires the resultant to satisfy F2F1RF1+F2|F_2 - F_1| \leq R \leq F_1 + F_2, and since 140 N lies outside the range 50 N to 120 N, the result violates this inequality and is physically impossible.
Explanation: When checking a physics answer, it helps to distinguish between necessary conditions (things that must be true) and sufficient conditions (things that guarantee correctness). The parallelogram (or cosine) law tells you the resultant of two concurrent forces must lie between F2F1|F_2 - F_1| and F1+F2F_1 + F_2, corresponding to the extremes of α=180°\alpha = 180° and α=0°\alpha = 0° respectively. Here, those bounds are 12050=70 N|120 - 50| = 70\text{ N} and 120+50=170 N120 + 50 = 170\text{ N}. Since R=140 NR = 140\text{ N} falls strictly inside this range, the answer passes a meaningful sanity check — it is physically plausible. That's exactly what A captures, making it the most justified statement. B is the critical trap here. Passing both limiting-case checks tells you the formula structure behaves correctly at the boundaries, but it says nothing about whether you substituted α\alpha correctly or avoided an arithmetic error in the middle. Boundary checks are necessary, not sufficient — do not confuse the two. C contains a real physics insight (R90°=502+1202=130 NR_{90°} = \sqrt{50^2 + 120^2} = 130\text{ N}), but its conclusion is wrong. If 140 N>130 N140\text{ N} > 130\text{ N}, that simply means α<90°\alpha < 90°, which is perfectly valid. Nothing in the problem forbids that angle, so there is no reason to "reject" the answer. D misapplies the triangle inequality. The correct bounds are F2F1RF1+F2|F_2 - F_1| \leq R \leq F_1 + F_2, which gives 70 N70\text{ N} to 170 N170\text{ N} — not 50 N50\text{ N} to 120 N120\text{ N}. The 50 N and 120 N are the individual force magnitudes, not the resultant's bounds. Study tip: On statics problems, always run the α=0°\alpha = 0° and α=180°\alpha = 180° checks first — but remember they bound your answer, not prove it. A result inside the bounds is plausible; only a complete derivation confirms it.

Question 5

A dynamics student derives the velocity of a particle undergoing projectile motion (launched at speed v0v_0 and angle θ\theta from horizontal, neglecting air resistance) at time tt as: v(t)=(v0cosθ)2+(v0sinθgt)2v(t) = \sqrt{(v_0\cos\theta)^2 + (v_0\sin\theta - gt)^2} The student also reports that the minimum speed during the flight occurs at t=v0gt^* = \frac{v_0}{g} and equals vmin=0v_{\min} = 0.

Using limiting cases and physical reasoning to check the reported minimum speed, which of the following conclusions is correct?

  1. The reported minimum speed vmin=0v_{\min} = 0 is incorrect only for θ<45\theta < 45^\circ; for θ45\theta \geq 45^\circ the horizontal and vertical components are equal at the apex, allowing the total speed to reach zero, confirming the student's result for steeper launch angles.
  2. The reported minimum speed is correct for the special case θ=90\theta = 90^\circ (vertical launch), and the formula t=v0/gt^* = v_0/g is valid for all launch angles because sinθ\sin\theta cancels out when differentiating v(t)v(t) to find the minimum.
  3. The reported minimum speed vmin=0v_{\min} = 0 is incorrect. At t=v0sinθ/gt^* = v_0\sin\theta/g (the apex), the vertical velocity component is zero but the horizontal component v0cosθv_0\cos\theta remains nonzero (for θ90\theta \neq 90^\circ), so vmin=v0cosθ>0v_{\min} = v_0\cos\theta > 0. The student's error is using t=v0/gt^* = v_0/g instead of t=v0sinθ/gt^* = v_0\sin\theta/g, and conflating zero vertical velocity with zero total speed. (correct answer)
  4. The formula for v(t)v(t) fails dimensional analysis because the argument of the square root mixes squared velocity terms with a squared acceleration-time product g2t2g^2t^2, making the expression dimensionally inconsistent and invalidating any conclusions drawn from it.
Explanation: Whenever you see a question about projectile motion extrema, train yourself to analyze each velocity component separately before drawing conclusions about total speed. The speed can only equal zero if every component simultaneously equals zero — a much stricter condition than just one component vanishing. At the apex of projectile motion, the vertical component vy=v0sinθgtv_y = v_0\sin\theta - gt equals zero, giving the correct apex time t=v0sinθgt^* = \frac{v_0\sin\theta}{g}. However, the horizontal component vx=v0cosθv_x = v_0\cos\theta is constant throughout the flight (no air resistance means no horizontal acceleration). So the minimum speed is vmin=(v0cosθ)2+02=v0cosθv_{\min} = \sqrt{(v_0\cos\theta)^2 + 0^2} = v_0\cos\theta, which is only zero when θ=90\theta = 90^\circ. This confirms C is correct: the student made two linked errors — using t=v0/gt^* = v_0/g (missing the sinθ\sin\theta factor) and then incorrectly concluding that zero vertical velocity implies zero total speed. A is wrong because the condition for zero total speed has nothing to do with whether θ45\theta \geq 45^\circ. The horizontal component persists at any angle except 9090^\circ, so vmin=0v_{\min} = 0 fails for all non-vertical launches. B is wrong on two counts: sinθ\sin\theta does not cancel when differentiating v(t)v(t) — it remains in the apex time formula — and t=v0/gt^* = v_0/g is only correct when θ=90\theta = 90^\circ. D is wrong because gtgt carries units of m/s (acceleration × time = velocity), so (gt)2(gt)^2 has units of m2/s2\text{m}^2/\text{s}^2, perfectly consistent with the other squared-velocity terms. The formula is dimensionally sound. Study tip: Always check limiting cases — set θ=90\theta = 90^\circ and θ=0\theta = 0^\circ to instantly expose errors in projectile motion formulas.

Question 6

A student analyzes a particle in plane curvilinear motion and derives the normal component of acceleration as an=v2ρa_n = \frac{v^2}{\rho}, yielding units check: (m/s)2m=m/s2\frac{(\text{m/s})^2}{\text{m}} = \text{m/s}^2. The student then applies this to a specific problem and reports an=8.5 m/s2a_n = -8.5\text{ m/s}^2.

Which of the following represents the best solution-checking practice for evaluating this reported result?

  1. The dimensional check is valid and confirms the formula structure, but the reported negative value an=8.5 m/s2a_n = -8.5\text{ m/s}^2 is physically unreasonable. Because an=v2/ρa_n = v^2/\rho is a magnitude — with both v2v^2 and ρ\rho strictly positive — a negative result indicates a sign or direction-convention error in the computation that the unit check cannot detect. (correct answer)
  2. The negative value is acceptable and physically meaningful: while the scalar magnitude v2/ρv^2/\rho is positive by definition, in a signed coordinate system the normal acceleration component can be expressed as negative when the center of curvature lies in the negative normal direction, so the sign simply reflects the chosen axis orientation.
  3. The dimensional check is the most critical verification step; since it confirms units of m/s², both the formula and the numerical result 8.5 m/s2-8.5\text{ m/s}^2 are validated. For intermediate-level curvilinear-motion problems, a successful unit check is generally sufficient to conclude the computation is correct.
  4. The result should be further checked by confirming that an|a_n| does not exceed the tangential acceleration ata_t in magnitude, because the normal component is geometrically bounded by the tangential component for any physically realizable curved path at non-constant speed.
Explanation: Whenever you encounter a problem involving curvilinear motion, you need to distinguish between formula validation (what a units check confirms) and physical reasonableness (what a units check cannot confirm). These are two separate layers of verification. The formula an=v2/ρa_n = v^2/\rho involves only squared speed and radius of curvature. Since v20v^2 \geq 0 always and ρ>0\rho > 0 by definition (it's a geometric length), the ratio is strictly non-negative. Reporting an=8.5 m/s2a_n = -8.5 \text{ m/s}^2 as a magnitude violates this constraint — the negative sign signals a computation error, likely a direction-convention mistake or an algebraic sign error, that slipped through undetected. Answer A correctly identifies both points: the units check is legitimate and confirms formula structure, but it operates independently of sign validity and cannot catch this class of error. Answer B introduces a plausible-sounding but subtly wrong idea. In a signed coordinate framework, vector components can be negative, but an=v2/ρa_n = v^2/\rho specifically defines the magnitude of the normal acceleration — it is not a signed component expression. Mixing these concepts is a common trap. Answer C overstates the power of dimensional analysis. Units confirm that your formula is dimensionally consistent; they say nothing about whether numerical values, signs, or physical constraints are satisfied. A units check passing is necessary but never sufficient. Answer D invents a constraint that does not exist. There is no geometric or physical rule bounding an|a_n| relative to at|a_t|; these components are independent. Study tip: Always layer your checks — units first, then sign/direction conventions, then order-of-magnitude reasonableness. A clean units check is just the starting point, not the finish line.

Question 7

A student solves a statics problem involving a simply supported beam and reports the reaction at the left support as RA=450 NR_A = 450\text{ N} and at the right support as RB=200 NR_B = 200\text{ N} for a single downward point load of P=600 NP = 600\text{ N} applied somewhere along the beam. The student checks moment equilibrium about one point and confirms it is satisfied. Which statement best identifies the most important additional check the student should perform and its implication?

  1. The student should verify that the ratio RA/RB=450/200=2.25R_A/R_B = 450/200 = 2.25 is physically reasonable by confirming that the load PP is located closer to support AA than to support BB, since a larger reaction at AA requires the load to be nearer to AA; if this geometric condition holds, the solution is confirmed.
  2. The student should verify moment equilibrium about the other support point to obtain a second independent equation, which when combined with the first moment equation uniquely confirms both reactions; checking force equilibrium is redundant because it is algebraically dependent on the two moment equations.
  3. The student should check that both reactions are positive, confirming the assumed directions are correct; since RA=450 N>0R_A = 450\text{ N} > 0 and RB=200 N>0R_B = 200\text{ N} > 0, both directions are confirmed and the solution is physically consistent with a simply supported beam under a downward load.
  4. The student should verify force equilibrium in the vertical direction: RA+RB=PR_A + R_B = P requires 450+200=650 N600 N450 + 200 = 650\text{ N} \neq 600\text{ N}. This check reveals that the answers are wrong, since confirming moment equilibrium about a single point does not guarantee force equilibrium is also satisfied — both independent equations must hold simultaneously. (correct answer)
Explanation: Whenever you solve a statics problem with a simply supported beam, remember that equilibrium requires two independent conditions to be satisfied simultaneously: the sum of all forces equals zero and the sum of all moments equals zero. Checking only one condition never fully validates your solution. Here, the student reports RA=450 NR_A = 450\text{ N} and RB=200 NR_B = 200\text{ N} for a single downward load P=600 NP = 600\text{ N}. The critical vertical force check is straightforward: Fy=0\sum F_y = 0 requires RA+RB=PR_A + R_B = P, meaning 450+200=650 N450 + 200 = 650\text{ N}, but the applied load is only 600 N600\text{ N}. Since 650600650 \neq 600, the solution is wrong, and no amount of moment-checking around a single point can rescue it. This is why D is correct — it identifies the violated equation and explains precisely why the error went undetected. Choice A is tempting but flawed: confirming the load's geometric position is a reasonableness check, not a mathematical verification. A solution can seem geometrically plausible while still violating equilibrium. Choice B contains a subtle misconception: for a simply supported beam with a single point load, force equilibrium and the two moment equations are not all independent — in fact, checking moments about both supports plus force equilibrium gives three equations for two unknowns, where any two imply the third. Force equilibrium is never truly redundant; it's the simplest and most direct check. Choice C is incomplete — positive values confirm assumed directions but say nothing about whether the magnitudes are actually correct. Your strategy: always run both checksF=0\sum F = 0 and M=0\sum M = 0 — before accepting any reaction solution. The arithmetic check RA+RB=PR_A + R_B = P takes five seconds and catches errors that moment equations alone will miss.