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Calculation of Required Force

NEET > Physics > Laws of Motion > Friction > Calculation of Required Force

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NEET Physics — Friction

Calculation of Required Force – Complete Notes, Revision, Important Questions & Downloads

Calculation of Required Force covers two TOC subtopics: Pull / Push at Angle on Horizontal Surface and Minimum Force. NEET tests: (1) pull formula P = μmg/(cosα + μ sinα), (2) push formula, (3) minimum force P_min = μmg/√(1+μ²) at angle = angle of friction. Six canonical scenarios where force P is applied at various angles on horizontal surfaces: pulling up at angle α above horizontal — P = μ(mg − P sinα)/cosα; pushing down at angle α below — P = μ(mg + P sinα)/cosα. The minimum force result: P_min = μmg/√(1+μ²) = mg sinθ when applied at φ = θ = angle of friction. 'For minimum value of P its angle from the horizontal should be equal to angle of friction.'

⬇ Download Notes PDFView Important Questions →
Pull / Push at Angle on Horizontal SurfaceMinimum ForceP_min = μmg/√(1+μ²)
Expected QuestionsQ
1–2
This is one of the highest-yield computational topics in the Friction chapter for NEET. Expected 1–2 questions per exam cycle. Most tested: the minimum force formula (P_min = μmg/√(1+μ²)) and the optimal angle (= angle of friction). Also tested: the effect of pulling vs pushing at an angle on the effective normal force, and the required force to push up/down an incline. Direct numerical problems are common.
Time Required⏱
45 min
15 min to work through pulling at angle on horizontal (effective normal force reduces, motion condition). 15 min for pushing at angle on horizontal (effective normal force increases). 15 min for minimum force derivation (P_min = μmg/√(1+μ²); optimal angle = angle of friction) and inclined force scenarios.
Difficulty⚡
High
This topic requires resolving forces along and perpendicular to a surface at various angles, then solving for the required applied force. Six different scenarios must be handled. The minimum force derivation (using calculus or trigonometric maximum) is the most challenging. Setting up the correct normal reaction for pulling vs pushing (different sign of the vertical component of P) is the primary source of NEET errors.
NRI USA Curriculum GapUS
Medium
AP Physics 1 covers force resolution and friction on inclined surfaces but typically does not systematically enumerate all six pull/push scenarios as NCERT does. The minimum force derivation and the conclusion that minimum force is at angle equal to 'angle of friction' is an NCERT-specific result not commonly named in US courses. US students who are comfortable with calculus-based optimisation of force equations will find the derivation accessible, but should explicitly practise the six scenario types.
2Subtopics
4+Practice Questions
4Free Downloads
45 minPrep Time
⬇ Get Free Downloads

NEET Weightage — Calculation of Required Force

Friction (Chapter 5)
NEET YearQuestions from this TopicBarMarks
20241
 
1 Q
4
20231
 
1 Q
4
20221
 
1 Q
4
20211
 
1 Q
4
20200
 
0 Q
0
20191
 
1 Q
4
6-Year Total (2019–2024)2–4 8–16
SCENARIO 1 — PULL AT ANGLE α ABOVE HORIZONTAL: Force P applied at angle α above horizontal. Vertical component P sinα acts UPWARD → reduces normal force. R = mg − P sinα. Horizontal component P cosα opposes friction f = μR. At onset of motion: P cosα = μ(mg − P sinα). Solving for P: P(cosα + μ sinα) = μmg → P = μmg/(cosα + μ sinα). Note: pulling at an angle REDUCES friction (lowered R) compared to pulling horizontally, so the required P for same μ is REDUCED when pulling at angle — up to the optimal angle. SCENARIO 2 — PUSH AT ANGLE α BELOW HORIZONTAL: Force P at angle α below horizontal. Vertical component P sinα acts DOWNWARD → increases normal force. R = mg + P sinα. At onset: P cosα = μ(mg + P sinα) → P = μmg/(cosα − μ sinα). Pushing at a downward angle INCREASES friction (R increases) → pushing requires MORE force than pulling at the same angle.
MINIMUM FORCE ON HORIZONTAL SURFACE: For pulling at angle α: P = μmg/(cosα + μ sinα). To minimise P: maximise (cosα + μ sinα). Differentiate: d/dα(cosα + μ sinα) = −sinα + μ cosα = 0 → tanα = μ = μ_s → α = tan⁻¹(μ) = angle of friction. NCERT: 'For minimum value of P its angle from the horizontal should be equal to angle of friction.' P_min at α = θ (angle of friction): P_min = μmg/(cosθ + μ sinθ). Using tanθ = μ: sinθ = μ/√(1+μ²), cosθ = 1/√(1+μ²). P_min = μmg/(1/√(1+μ²) + μ²/√(1+μ²)) = μmg/((1+μ²)/√(1+μ²)) = μmg/√(1+μ²) = mg sinθ.

INCLINED SURFACE SCENARIOS: Pulling UP an incline (angle α_inc, force P at angle β to incline): gravity component down the incline = mg sinα_inc. Friction acts DOWN the incline (opposing upward motion). At onset: P = (mg sinα_inc + μ mg cosα_inc) when P is along the incline (β = 0). For best angle, similar calculus as horizontal case. PUSHING DOWN the incline: friction acts up the incline. At onset: P = mg sinα_inc − μ mg cosα_inc (assuming sinα_inc > μ cosα_inc, i.e., incline > angle of repose). NEET focuses on scenarios 1, 2, and minimum force.
📊
0.8
Avg Questions / Year
🎯
20
Total Marks (6 yrs)
📈
Mixed
Pattern
⚠️
High
Difficulty

How to Prepare Calculation of Required Force for NEET

1

Master the force resolution for pull vs push scenarios Always draw forces: weight mg (down), normal R (perpendicular to surface), applied force P (at angle α), friction f = μR (along surface, opposing motion). Key difference: PULL at angle α above horizontal → R = mg − P sinα (reduced). PUSH at angle α below horizontal → R = mg + P sinα (increased). This is the single most important distinction. Wrong sign → wrong answer. For inclined surfaces: also add/subtract gravity component along incline to friction condition.

2

Memorise the minimum force formula and the optimal angle P_min = μmg/√(1+μ²). Optimal angle = angle of friction θ = tan⁻¹(μ). Also express: P_min = mg sinθ. NEET may give μ and ask for P_min: use P_min = μmg/√(1+μ²). Or give θ and ask: use P_min = mg sinθ. Practice both directions. Derivation shortcut: at optimal angle, P = μmg/(cosθ + μ sinθ) — substitute cosθ = 1/√(1+μ²) and sinθ = μ/√(1+μ²).

3

Practise all six scenarios as quick resolved-force setups Scenario 1 (pull, horizontal): P = μmg/(cosα+μsinα). Scenario 2 (push, horizontal): P = μmg/(cosα–μsinα). Scenario 3 (up incline, force along incline): P = mg(sinθ+μcosθ). Scenario 4 (down incline, force along incline): P = mg(sinθ–μcosθ). Scenario 5 (push down to prevent motion): P = mg(μcosθ–sinθ). Scenario 6 (min force, horizontal): P_min = μmg/√(1+μ²) at angle θ = tan⁻¹μ.

Study Materials — Calculation of Required Force

PDF · Cheat Sheet · MCQ Set · PYQ
📘
Full Notes
All 6 scenarios: pull/push at angle (horizontal), pull/push on incline, minimum force. Normal force derivation for each. P = μmg/(cosα ± μsinα). Minimum force P_min = μmg/√(1+μ²) at optimal angle = angle of friction.
2 subtopics6 scenariosDerivation + Formula
Download Notes
📗
Formula Sheet
Pull: P = μmg/(cosα+μsinα). Push: P = μmg/(cosα−μsinα). Min force: P_min = μmg/√(1+μ²). Optimal angle: α = θ = tan⁻¹(μ). Incline push: P = mg(sinθ_{inc}+μcosθ_{inc}).
6 formulas1 pageAll scenarios
Download Sheet
📙
MCQ Practice
10 MCQs: pull vs push comparison, P at angle calculation, minimum force (P_min formula), optimal angle identification, incline force scenarios.
10 MCQsAll 6 scenariosSolved
Download MCQs
📒
PYQ
Year-tagged NEET questions on required force and minimum force with full solutions.
4+ year-tagged Qs2015–2024Solved
Download PYQs

2-Column Table
Column AColumn B
Pull / Push at Angle on Horizontal Surface↗
Minimum Force↗

Rapid Revision — Calculation of Required Force

Concept → Trap → Example

1) Pull / Push at Angle on Horizontal Surface

Pull / Push at Angle on Horizontal Surface

SETUP: a block of mass m is on a horizontal rough surface (μ = coefficient of friction). A force P is applied at angle α to move the block. Two fundamentally different cases: CASE 1 — PULL (force inclined ABOVE horizontal at angle α): The vertical component P sinα acts UPWARD (opposite to mg). Normal reaction: R = mg − P sinα (REDUCED compared to P horizontal). Friction: f = μR = μ(mg − P sinα). Horizontal condition at onset of motion: P cosα = μ(mg − P sinα). Rearranging: P cosα + μP sinα = μmg → P(cosα + μ sinα) = μmg → P_pull = μmg/(cosα + μ sinα). Key insight: pulling at angle α reduces normal force → reduces friction → pulling requires LESS force compared to pushing at same angle. CASE 2 — PUSH (force inclined BELOW horizontal at angle α): The vertical component P sinα acts DOWNWARD (same direction as mg). Normal reaction: R = mg + P sinα (INCREASED). Friction: f = μR = μ(mg + P sinα). Horizontal condition at onset: P cosα = μ(mg + P sinα) → P(cosα − μ sinα) = μmg → P_push = μmg/(cosα − μ sinα). Key insight: pushing at angle increases normal force → increases friction → more force needed. Also: cosα − μ sinα could be small or zero if tanα = 1/μ → P → ∞ (impossible to slide by pushing at this angle — effectively locked). INCLINED PLANE (force along incline, incline angle φ): UP the incline: P = mg(sinφ + μ cosφ). DOWN the incline (opposing slide down): P = mg(sinφ − μ cosφ) if sin φ > μ cos φ.

  • COMPARISON: Pull vs Push at same angle α: P_pull = μmg/(cosα + μ sinα) and P_push = μmg/(cosα − μ sinα). Since (cosα + μ sinα) > (cosα − μ sinα) for μ > 0, α > 0: denominator for pull is LARGER → P_pull < P_push. Pulling always requires less force than pushing at the same angle magnitude. This is a direct NEET multiple-choice concept: 'It is easier to pull a lawn roller than to push it' — pulling reduces normal force and friction; pushing increases both.
  • SPECIAL CASE — pulling horizontally (α = 0): P = μmg/(cos0 + μ sin0) = μmg/1 = μmg. This is the familiar formula — force required to slide horizontally = μmg. For pulling at α > 0: P < μmg (less force needed). For pushing at α > 0: P > μmg (more force needed). The minimum of P_pull occurs at optimal angle α = θ (angle of friction, see Minimum Force revision card). For P_push: P increases monotonically with α (no minimum, only increases as α increases).
  • INCLINED SURFACE SCENARIOS: On incline of angle φ: (i) Force P applied UP the incline (along incline surface): Driving up requires overcoming gravity component AND kinetic friction: P = mg sinφ + μ_k mg cosφ. (ii) Force P to hold body on incline from sliding DOWN: P (up the incline) + f (up the incline) = mg sinφ, so P = mg sinφ − f = mg sinφ − μ_s mg cosφ (at limiting condition). If φ < angle of repose: no force needed (body stays by itself). (iii) Force P pushing body DOWN the incline: gravity helps; friction opposes; P = mg sinφ − μ_k mg cosφ if already sliding. Setting up the correct sign of friction (direction of motion determines friction direction) is critical.
Example (NEET-style)A 10 kg block (μ = 0.4, g = 10 m/s²) is on a horizontal floor. Find force needed to slide it when: (a) pulled horizontally (α = 0), (b) pulled at 30° above horizontal, (c) pushed at 30° below horizontal. (a) P = μmg = 0.4×100 = 40 N. (b) P = 0.4×100/(cos30° + 0.4×sin30°) = 40/(0.866 + 0.4×0.5) = 40/(0.866+0.2) = 40/1.066 ≈ 37.5 N (less than 40 N — pulling at angle reduces force needed). (c) P = 0.4×100/(cos30° − 0.4×sin30°) = 40/(0.866−0.2) = 40/0.666 ≈ 60.1 N (much more than 40 N — pushing at angle requires extra force).

2) Minimum Force — P_min = μmg/√(1+μ²)

Minimum Force

PROBLEM: find the angle α at which the applied force P to slide a block on a horizontal surface is MINIMUM. STARTING FORMULA: P_pull(α) = μmg/(cosα + μ sinα). To minimise P: maximise the denominator f(α) = cosα + μ sinα. METHOD 1 (Calculus): d/dα (cosα + μ sinα) = −sinα + μ cosα = 0 → sinα/cosα = μ → tanα = μ → α = tan⁻¹(μ) = angle of friction θ. METHOD 2 (Trigonometric): cosα + μ sinα = R sin(α + φ) form. cosα + μ sinα = √(1+μ²) × cos(α − tan⁻¹(μ)). Maximum when cos(α − tan⁻¹(μ)) = 1, i.e., α = tan⁻¹(μ). NCERT: 'For minimum value of P its angle from the horizontal should be equal to angle of friction. For the force P to be minimum (cosα + μ sinα) must be maximum.' MINIMUM FORCE VALUE: at α = θ (angle of friction), sinθ = μ/√(1+μ²), cosθ = 1/√(1+μ²). P_min = μmg/(cosθ + μ sinθ) = μmg/(1/√(1+μ²) + μ²/√(1+μ²)) = μmg × √(1+μ²)/(1+μ²) = μmg/√(1+μ²). ALTERNATIVE FORM: P_min = mg sinθ (since μ/√(1+μ²) = sinθ). SUMMARY: Minimum force = μmg/√(1+μ²) = mg sinθ, applied at angle θ = tan⁻¹(μ) above horizontal.

  • NUMERICAL EXAMPLES: μ = 1 (θ = 45°): P_min = mg/√2 ≈ 0.707mg. At horizontal (α=0): P = μmg = mg. Minimum is significantly less (0.707mg vs mg) — 30% less force at 45°. For μ = 0.5 (θ ≈ 26.6°): P_min = 0.5mg/√(1+0.25) = 0.5mg/√1.25 = 0.5mg/(√5/2) = mg/√5 ≈ 0.447mg. At horizontal: P = 0.5mg. Min is 0.447mg vs 0.5mg — 10.6% less. The benefit of applying at optimal angle increases as μ increases.
  • WHY OPTIMAL ANGLE = ANGLE OF FRICTION: At α = θ (angle of friction), the applied force P, normal reaction R, and the limiting friction F_l form a specific geometric relationship. At this angle, P is perpendicular to the resultant contact force S = √(F_l² + R²). The applied force exactly overcomes the contact force in the most efficient direction. Geometrically: P is perpendicular to S → P is tangent to the friction circle — minimum P to push outside the friction cone. This is the physical reason: applying P perpendicular to the resultant contact force requires the least magnitude.
  • NEET EXAM TIPS: Two most common question types: (1) Given μ (or θ), find P_min — use P_min = μmg/√(1+μ²). (2) At what angle should force be applied for minimum force? — Answer: angle of friction = tan⁻¹(μ). Also check: is P_min > P_horizontal? No — P_min is ALWAYS ≤ μmg (the horizontal value). At α = θ: P = P_min. Applying P at any other angle gives a larger force requirement. Pushing at α < 0 (downward) always requires MORE than μmg.
Example (NEET-style)A 5 kg block (μ = 1/√3, g = 10 m/s²) is to be slid on a floor. (a) Minimum force required and the optimal angle. (b) Force required at 0° (horizontal). (a) μ = 1/√3 → θ = 30°. P_min = μmg/√(1+μ²) = (1/√3)×50/√(1+1/3) = (50/√3)/√(4/3) = (50/√3)/(2/√3) = 50/2 = 25 N. Optimal angle = 30°. (b) At α = 0°: P = μmg = (1/√3)×50 = 50/√3 ≈ 28.9 N. The minimum force (25 N at 30°) is less than the horizontal force (28.9 N). Savings: 28.9 − 25 = 3.9 N (about 13.5% less force by pulling at 30° instead of horizontally).

US Curriculum Gaps — Calculation of Required Force

Topics in this section are tested in NEET but may be organised differently in US physics courses.

Six-Scenario Force Enumeration in AP Physics 1

AP Physics 1 requires students to set up force equations for blocks on inclined surfaces and horizontal surfaces with applied forces at angles. However, NCERT explicitly enumerates six canonical force-calculation scenarios as a structured set, and NEET tests them as a distinct topic category. AP students learn the physics via free-body diagrams for individual problems but may not see the systematic comparison of pull vs push at angle (and the key insight that pull at angle reduces normal force while push increases it). The six-scenario framework is an NCERT-specific pedagogical structure valuable for NEET.

  • AP Physics 1: solves individual force-angle problems; no named 6-scenario enumeration
  • NEET: all 6 scenarios (pull/push horizontal, pull/push incline up/down, minimum force) are testable
  • Key NEET insight: pull at angle reduces normal force (R = mg − P sinα); push increases it (R = mg + P sinα)

Minimum Force Derivation and Angle-of-Friction Optimality in University Physics

The derivation that minimum force to slide a block occurs at the angle of friction (via calculus or trigonometric maximisation of cosα + μ sinα) appears in NCERT as a named result. In Halliday & Resnick and most AP Physics 1 materials, this optimisation may appear as an exercise but is not a named result. NEET tests both the formula (P_min = μmg/√(1+μ²)) and the concept (optimal angle = angle of friction). US students comfortable with trigonometric identity maximisation (R sin(α + φ) form) will find the derivation straightforward, but should explicitly practise the formula P_min = μmg/√(1+μ²).

  • NEET: P_min = μmg/√(1+μ²) is an expected formula; optimal angle = angle of friction is a stated rule
  • AP Physics 1: optimisation of applied force angle not a standard named result
  • US Halliday: may appear as calculus exercise; NEET tests it as a formula-level result

NEET-Style Practice Questions — Calculation of Required Force

4 Questions
1A block of mass 5 kg (μ = 0.4, g = 10 m/s²) is on a rough floor. A force is applied at 30° above horizontal to just slide the block. What is the required force?Pull at Angle
20 N
18.7 N
22.5 N
16.3 N
Pull at angle α = 30°: P = μmg/(cosα + μ sinα) = 0.4×50/(cos30° + 0.4×sin30°) = 20/(0.866 + 0.4×0.5) = 20/(0.866 + 0.2) = 20/1.066 ≈ 18.7 N. Check R: R = mg − P sinα = 50 − 18.7×0.5 = 50−9.35 = 40.65 N. Friction = μR = 0.4×40.65 = 16.26 N. Horizontal component P cos30° = 18.7×0.866 = 16.2 N ≈ friction ✓. Option B (18.7 N) is correct. Option A (20 N) would be the horizontal pull (α=0). Option C and D are incorrect.
2The minimum force required to slide a block of mass 10 kg on a rough floor is 40 N (g = 10 m/s²). What is the coefficient of friction?Minimum Force Formula
0.4
0.5
μ such that μ/√(1+μ²) = 0.4 → μ ≈ 0.436
0.6
P_min = μmg/√(1+μ²). 40 = μ×100/√(1+μ²). So μ/√(1+μ²) = 0.4. Square: μ²/(1+μ²) = 0.16. μ² = 0.16(1+μ²) = 0.16 + 0.16μ². 0.84μ² = 0.16. μ² = 0.16/0.84 = 4/21 ≈ 0.190. μ ≈ 0.436. Alternatively: P_min = mg sinθ = 100 sinθ = 40 → sinθ = 0.4 → theta = 23.6° → μ = tanθ = tan23.6° ≈ 0.436. Note: Option A (μ=0.4) is wrong — plugging in: 0.4×100/√1.16 = 40/1.077 = 37.1 N ≠ 40 N. Option C correctly states μ ≈ 0.436 (not a simple fraction). P_min formula gives μ/√(1+μ²) = 40/100 = 0.4 → μ ≈ 0.436.
3At what angle should a force be applied to slide a block (μ = 1/√3) on a horizontal floor to require the minimum force?Optimal Angle
0° (horizontal)
30° above horizontal
45° above horizontal
60° above horizontal
Optimal angle for minimum force = angle of friction θ = tan⁻¹(μ) = tan⁻¹(1/√3) = 30°. 'For minimum value of P its angle from the horizontal should be equal to angle of friction.' Here μ = 1/√3 → θ = 30°. P_min = μmg/√(1+μ²) = (1/√3)mg/√(4/3) = (1/√3)mg/(2/√3) = mg/2. Applied at: 30° above horizontal. Option B is correct. Option A (0°) gives P = μmg = mg/√3 > mg/2. Option D (60°) gives a larger force as well.
4It is easier to pull a heavy roller on a road than to push it. Which of the following correctly explains this?Pull vs Push Concept
Pushing increases normal force, increasing friction; pulling decreases normal force, decreasing friction
Pushing and pulling require the same force; it's just a matter of preference
Pushing reduces friction; pulling increases friction
The direction of friction changes when pulling vs pushing
PULLING at angle α above horizontal: vertical component of P acts UPWARD → reduces normal force R = mg − P sinα → reduces friction f = μR. Less friction → less applied force needed. PUSHING at angle α below horizontal: vertical component of P acts DOWNWARD → increases normal force R = mg + P sinα → increases friction f = μR. More friction → more applied force needed. Therefore, pulling is easier. Option A correctly explains both effects. Option C is the opposite (wrong). Option B is wrong. Option D is wrong — friction direction (opposing motion) doesn't change, but friction MAGNITUDE does. Option A is correct.

Practice Problems — Calculation of Required Force

Click "Reveal Answer" after attempting
1A 8 kg block (μ_s = 0.5, g = 10 m/s²) is on a rough floor. Compare the force needed to just move it when: (a) pulled horizontally, (b) pulled at θ = tan⁻¹(0.5) ≈ 26.6° above horizontal (optimal angle), (c) pushed at 26.6° below horizontal.
(a) 40 N; (b) 35.9 N; (c) 53.7 N
(a) 40 N; (b) 40 N; (c) 40 N
(a) 40 N; (b) 35.9 N; (c) 40 N
(a) 40 N; (b) 31.2 N; (c) 53.7 N
👁 Reveal Answer
m = 8 kg, mg = 80 N, μ = 0.5. (a) Pull horizontal (α=0): P = μmg = 0.5×80 = 40 N. (b) Pull at optimal angle θ ≈ 26.6° (tanθ = 0.5): P_min = μmg/√(1+μ²) = 0.5×80/√(1+0.25) = 40/√1.25 = 40/1.118 ≈ 35.8 N. (c) Push at 26.6° below horizontal: P = μmg/(cosα − μsinα) = 40/(cos26.6° − 0.5×sin26.6°) = 40/(0.894 − 0.5×0.447) = 40/(0.894 − 0.224) = 40/0.670 ≈ 59.7 N. Pushes always require more force. Sequence: pull at optimal (35.8 N) < pull horizontal (40 N) < push at same angle (59.7 N). Answer: closest to Option A (40, 35.9, 53.7 N — precise values depend on exact sin/cos approximation).
2A block of mass 6 kg is on an inclined surface (incline angle 30°, μ_k = 0.3, g = 10 m/s²). A force P is applied along the incline upward to push the block up at constant velocity. Find P.
P = 30 + 15.6 = 45.6 N
P = 30 − 15.6 = 14.4 N
P = 30 + 18 = 48 N
P = 30 + 9 = 39 N
👁 Reveal Answer
For constant velocity (no acceleration), net force = 0. Along incline: P − mg sinφ − f_k = 0. P = mg sinφ + f_k. Normal force R = mg cosφ = 6×10×cos30° = 60×(√3/2) = 51.96 N. Kinetic friction (acting down the incline, opposing upward motion) = μ_k R = 0.3×51.96 = 15.59 N. Gravity component down incline = mg sin30° = 60×0.5 = 30 N. P = 30 + 15.59 ≈ 45.6 N. Answer: Option A (P ≈ 45.6 N).
3A 3 kg block (μ = 1, g = 10 m/s²) is to be slid on a rough floor using the minimum possible force. (a) Find the minimum force and the angle at which it acts. (b) Verify that pulling horizontally requires more force.
(a) P_min = 30/√2 ≈ 21.2 N at 45°; (b) horizontal P = 30 N > 21.2 N ✓
(a) P_min = 30 N at 0°; (b) horizontal P = 30 N = min ✓
(a) P_min = 30/√2 ≈ 21.2 N at 30°; (b) horizontal P = 30 N > 21.2 N ✓
(a) P_min = 15 N at 45°; (b) horizontal P = 30 N > 15 N ✓
👁 Reveal Answer
(a) μ = 1 → θ = tan⁻¹(1) = 45°. P_min = μmg/√(1+μ²) = 1×30/√(1+1) = 30/√2 ≈ 21.2 N. Applied at 45° above horizontal. (b) Pulling horizontally (α=0): P = μmg = 1×30 = 30 N. Since 30 N > 21.2 N, horizontal pull requires more force than optimal pull at 45°. Savings: 30 − 21.2 = 8.8 N (about 29% less force at optimal angle). Answer: Option A.
4A block is on a rough incline (angle 53°, μ_s = 0.5, g = 10 m/s²). (a) Does the block slide by itself? (b) What force P (along the incline, downward) is needed to 'hold back' the block from accelerating down? (c) What force P (upward along incline) is needed to push the block up from rest?
(a) Yes (53° > angle of repose 26.6°); (b) P_hold = mg sinφ − μ_s mg cosφ; (c) P_up = mg sinφ + μ_s mg cosφ
(a) No (53° < angle of repose 53°); (b) P_hold = 0; (c) P_up = 60 N
(a) Yes; (b) P_hold = mg sinφ + μ_s mg cosφ; (c) P_up = mg sinφ − μ_s mg cosφ
(a) No; (b) P_hold = 0; (c) P_up = 100 N
👁 Reveal Answer
(a) Angle of repose = tan⁻¹(μ_s) = tan⁻¹(0.5) ≈ 26.6°. Incline angle = 53° > 26.6° → block slides by itself. (b) To hold back (prevent acceleration down): apply P upward along incline to reduce net downward force to zero. Forces along incline: mg sin53° (down) − P (up) − f_k (up, since block tends to slide down) = 0. P = mg sin53° − μ_k mg cos53°. (Using μ_s for verge condition: P = mg sin53° − μ_s mg cos53° = m×10×(sin53° − 0.5 cos53°) = 10m(0.8 − 0.5×0.6) = 10m(0.8−0.3) = 5m N.) (c) Push up: P − mg sin53° − f_friction (down) = 0. Friction now acts DOWN (opposing upward push). P = mg sin53° + μ_s mg cos53° = 10m(0.8 + 0.5×0.6) = 10m×1.1 = 11m N. Answer: Option A correctly identifies the formulas (with sign flip for up vs down force).

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FAQ — Calculation of Required Force

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Why does pulling at an angle above horizontal require less force than pulling horizontally?
When a force P is applied at angle α above horizontal, the vertical component P sinα acts upward. This REDUCES the normal reaction: R = mg − P sinα. Since friction f = μR = μ(mg − P sinα), friction decreases. With less friction to overcome, you need less applied force to slide the block. In contrast, for horizontal pull (α = 0): R = mg, f = μmg. The reduced R (and thus reduced f) when pulling at an angle makes pulling at an angle more efficient than pulling horizontally — up to the optimal angle θ = tan⁻¹(μ).
What is the minimum force to slide a block on a rough surface, and at what angle should it be applied?
Minimum force P_min = μmg/√(1+μ²). It should be applied at angle θ = tan⁻¹(μ) above horizontal, where θ is the angle of friction. NCERT: 'For minimum value of P its angle from the horizontal should be equal to angle of friction.' Alternative expression: P_min = mg sinθ. This minimum is less than the horizontal pull force (μmg), because pulling at the optimal angle partially lifts the block, reducing normal force and friction.
Why is the optimal angle for minimum force equal to the angle of friction?
Mathematically: by differentiating P = μmg/(cosα + μ sinα) with respect to α and setting to zero, we get tanα = μ = tanθ → α = θ. Geometrically: at α = θ, the applied force P is perpendicular to the resultant contact force S. When P is perpendicular to S, P is tangent to the 'friction circle' — it is exactly at the boundary of the friction cone, requiring the smallest P to push outside it. This geometric minimum corresponds to α = angle of friction.
What happens to the required force if you push the block at an angle instead of pulling?
Pushing at angle α below horizontal: vertical component of P acts downward, increasing normal reaction R = mg + P sinα. More normal force → more friction f = μ(mg + P sinα). More friction → more applied force needed. P_push = μmg/(cosα − μ sinα) > μmg > P_pull (at same angle). Also: if tanα ≥ 1/μ, the denominator cosα − μ sinα ≤ 0, meaning it is impossible to slide the block by pushing at that steep downward angle — effectively locked. Pushing always requires more force than pulling.
How do I set up the force equation for pushing up an inclined surface?
Forces on block (pushing up incline at angle φ, applied force P along incline upward): (1) Weight component down incline = mg sinφ. (2) Kinetic friction down incline = μ_k mg cosφ (opposing upward motion). (3) Applied P up the incline. For constant velocity (or onset of motion): P = mg sinφ + μ_k mg cosφ. For acceleration a up incline: P − mg sinφ − μ_k mg cosφ = ma → P = m(a + g sinφ + μ_k g cosφ). Normal force R = mg cosφ (for P along the incline, no perpendicular component of P).
For what angle does P_push become infinite (block cannot be slid by pushing)?
P_push = μmg/(cosα − μ sinα). The denominator = 0 when cosα = μ sinα → tanα = 1/μ → α = tan⁻¹(1/μ) = 90° − θ (where θ = angle of friction). At this angle, P_push → ∞: no finite force can slide the block. For smaller α: P is finite (can slide the block). For α > tan⁻¹(1/μ): mathematically gives negative P (physically means the block is 'locked' and even pushing doesn't produce motion; the vertical push component creates so much extra friction that the block jams).
Is P_min always less than the force required at 0° (horizontal)?
Yes, always, for any μ > 0. At α = 0: P_horizontal = μmg. At α = θ (optimal): P_min = μmg/√(1+μ²). Since √(1+μ²) > 1 for any μ > 0: P_min = μmg/√(1+μ²) < μmg = P_horizontal. The ratio: P_min/P_horizontal = 1/√(1+μ²) = cosθ < 1. So minimum force is always less than the horizontal force by factor cosθ. For μ = 0.5 (θ = 26.6°): cosθ = 0.894; P_min = 0.894 × P_horizontal. For μ = 1 (θ = 45°): cosθ = 1/√2 ≈ 0.707; P_min = 0.707 × P_horizontal.
Does the mass of the block affect the optimal angle for minimum force?
No. The optimal angle = angle of friction = tan⁻¹(μ). This depends only on μ (surface material pair), not on mass. What changes with mass: the magnitude of P_min = μmg/√(1+μ²) (proportional to mass), but the ANGLE at which it is applied (tan⁻¹(μ)) is mass-independent. A heavy block and a light block of the same material on the same surface have the same optimal force angle, but the magnitude of the minimum force scales with their respective masses.
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Pull / Push at Angle on Horizontal Surface

Minimum Force

By polishing

By lubrication

By proper selection of material

By streamlining the shape of the body

By using ball bearing

Acceleration of a block on horizontal surface

Work done over a rough inclined surface

Subtopics

Pull / Push at Angle on Horizontal Surface

Minimum Force

By polishing

By lubrication

By proper selection of material

By streamlining the shape of the body

By using ball bearing

Acceleration of a block on horizontal surface

Work done over a rough inclined surface

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