Singly Reinforced Beam
Design & Analysis as per IS 456:2000 (LSM) — Neutral Axis, Moment of Resistance, Steel Area Calculation & Solved GATE Examples
Last Updated: March 2026
Key Takeaways 📌
- A singly reinforced beam (SRB) has steel reinforcement only in the tension zone — there is no compression steel. It is the most fundamental RCC member and the starting point for all beam design.
- At the ultimate limit state, the compressive force C in the concrete stress block equals the tensile force T in the steel — this force equilibrium determines the neutral axis depth xu.
- The moment of resistance Mu = C × lever arm = T × lever arm = 0.87fyAst(d − 0.42xu).
- IS 456 limits xu ≤ xu,max to ensure ductile under-reinforced failure. For Fe 415: xu,max/d = 0.48.
- The limiting (balanced) moment Mu,lim = maximum moment a singly reinforced section of given b and d can carry = 0.36fck × b × xu,max × (d − 0.42xu,max).
- If the applied Mu > Mu,lim: a singly reinforced section is insufficient — use a doubly reinforced beam or increase the section depth.
- For Fe 415, M20: Mu,lim = 2.76 bd² (N·mm, b and d in mm) — this is the most useful pre-computed value to memorise for GATE CE.
1. What is a Singly Reinforced Beam?
A singly reinforced beam is an RCC beam that has steel bars placed only in the tension zone — the zone of the cross-section where the net stress is tensile. For a simply supported beam under gravity loading, the tension zone is at the bottom (the beam sags), so the steel bars are placed near the bottom face. For a cantilever beam, the tension zone is at the top, so the steel goes near the top face.
The word "singly" refers to reinforcement on one side only — the tension side. There is no compression reinforcement in a singly reinforced beam. The compressive force that equilibrates the tension in the steel is carried entirely by the concrete in the compression zone.
Singly reinforced beams are used when the applied bending moment is moderate — when the section can carry the required moment using only the concrete's compressive capacity. If the moment is too large for the available concrete compression area to handle (i.e., the required neutral axis depth exceeds xu,max), a doubly reinforced beam (with compression steel added) is needed, or the section depth must be increased.
The geometry of a singly reinforced rectangular beam is characterised by four dimensions:
- b = breadth (width) of the beam [mm]
- D = overall depth of the beam [mm]
- d = effective depth = D − cover − stirrup diameter − main bar radius [mm]
- Ast = area of tension steel = n × (π/4) × φ² for n bars of diameter φ [mm²]
The effective depth d is the critical dimension for all design calculations — it is the distance from the compression face to the centroid of the tension reinforcement. For GATE CE problems, d is usually given directly. In practice, d = D − effective cover, where the effective cover accounts for the clear cover, stirrup diameter, and half the main bar diameter.
2. Stress and Strain Distribution at Ultimate
At the ultimate limit state — just before the beam fails — the following conditions exist in the cross-section:
Strain Distribution (IS 456 Cl. 38.1)
Strain varies linearly across the depth of the section (plane sections remain plane — Bernoulli's assumption applies even at ultimate for RCC).
Maximum compressive strain in concrete at the extreme compression fibre = εcu = 0.0035 (IS 456 — this is the crushing strain of concrete)
Strain in tension steel at ultimate:
εst = εcu × (d − xu) / xu
For the section to be under-reinforced: εst ≥ 0.87fy/Es + 0.002 (steel yields before concrete crushes)
For balanced section: εst = 0.87fy/Es + 0.002 exactly (both reach limits simultaneously)
Stress Distribution (IS 456 Equivalent Rectangular Block)
Compression zone (above neutral axis):
Actual stress: parabolic-rectangular (complex curve)
IS 456 equivalent: uniform stress of 0.36 fck over a depth of 0.42 xu from the compression face
Total compressive force: C = 0.36 fck × b × xu
Line of action of C: at 0.42xu/2 = 0.21xu... IS 456 places it at 0.42xu from the extreme compression fibre
Tension zone (below neutral axis):
Concrete below NA: cracked, carries zero stress
Steel bars: stress = 0.87 fy (design yield stress, for under-reinforced section)
Total tensile force: T = 0.87 fy × Ast
3. Force Equilibrium — Neutral Axis
At the ultimate limit state, the section is in equilibrium — the total compressive force C equals the total tensile force T (there is no net axial force on a pure bending member).
Neutral Axis Depth xu — From Force Equilibrium
C = T
0.36 fck × b × xu = 0.87 fy × Ast
xu = (0.87 fy × Ast) / (0.36 fck × b)
Or equivalently:
xu = 2.415 × (fy / fck) × (Ast / b)
This is the actual neutral axis depth for the given section. If xu ≤ xu,max → under-reinforced (acceptable). If xu > xu,max → over-reinforced (not permitted in IS 456 LSM).
Neutral Axis in Terms of Steel Percentage pt
Steel percentage: pt = 100 Ast / (bd)
Ast = pt × bd / 100
Substituting: xu/d = (0.87 fy / fck) × (pt / 100) / 0.36
xu/d = (pt / 100) × (0.87 fy) / (0.36 fck)
For Fe 415, M20: xu/d = (pt/100) × (0.87×415)/(0.36×20) = (pt/100) × 50.15
xu/d = 0.5015 pt
At balanced (xu/d = 0.48): pt,bal = 0.48/0.5015 = 0.957% ≈ 0.96%
4. Moment of Resistance
The moment of resistance of a singly reinforced beam section is the couple formed by the compressive force C and the tensile force T, separated by the lever arm z.
Moment of Resistance Mu (IS 456)
Taking moments of the internal forces about the line of action of the tensile force T:
Mu = C × z = 0.36 fck × b × xu × (d − 0.42 xu)
Or taking moments about the line of action of C:
Mu = T × z = 0.87 fy × Ast × (d − 0.42 xu)
Where lever arm z = d − 0.42 xu
Both expressions give the same Mu — use whichever is more convenient for the problem at hand.
The T formula is usually easier for design problems (when Ast is the unknown — substitute xu in terms of Ast).
The C formula is usually easier for analysis problems (when Ast is given — find xu first, then substitute).
Moment of Resistance — Compact Form
Substituting xu = 0.87fyAst / (0.36fckb) into the T formula:
Mu = 0.87fyAstd × [1 − (0.87fyAst) / (0.36fck × bd)]
Mu = 0.87 fy Ast d [1 − (fy Ast) / (fck b d)]
This is IS 456 Equation (a) from Annex G — the most compact design formula for a singly reinforced beam.
This is a quadratic in Ast and is used in design problems to find the required steel area.
5. Limiting Moment Mu,lim — Balanced Section
The limiting moment Mu,lim is the moment of resistance of a balanced (limiting) section — a section where xu = xu,max. It represents the maximum moment a singly reinforced section of given b and d can carry without exceeding the limiting neutral axis depth.
Mu,lim — Formula
Mu,lim = 0.36 fck × b × xu,max × (d − 0.42 xu,max)
Factoring out bd²:
Mu,lim = 0.36 × (xu,max/d) × fck × [1 − 0.42 × (xu,max/d)] × bd²
Mu,lim = Ru,lim × bd²
Where Ru,lim = 0.36 × (xu,max/d) × fck × [1 − 0.42 × (xu,max/d)]
Ru,lim Values for Common Grade Combinations ⭐ GATE
| Steel | Concrete | xu,max/d | Ru,lim (N/mm²) | Mu,lim |
|---|---|---|---|---|
| Fe 415 | M20 | 0.48 | 2.76 | 2.76 bd² N·mm |
| Fe 415 | M25 | 0.48 | 3.45 | 3.45 bd² N·mm |
| Fe 415 | M30 | 0.48 | 4.14 | 4.14 bd² N·mm |
| Fe 500 | M20 | 0.46 | 2.66 | 2.66 bd² N·mm |
| Fe 500 | M25 | 0.46 | 3.33 | 3.33 bd² N·mm |
| Fe 250 | M20 | 0.53 | 2.98 | 2.98 bd² N·mm |
Most important to memorise: Fe 415 + M20 → Mu,lim = 2.76 bd²
This combination is by far the most common in GATE CE problems.
Verification for Fe 415, M20: Ru,lim = 0.36 × 0.48 × 20 × (1 − 0.42×0.48) = 3.456 × (1 − 0.2016) = 3.456 × 0.7984 = 2.758 ≈ 2.76 ✓
Balanced Steel Area Ast,bal
The steel area at the balanced condition:
0.36 fck × b × xu,max = 0.87 fy × Ast,bal
Ast,bal = 0.36 fck × b × xu,max / (0.87 fy)
For Fe 415, M20: Ast,bal = (0.36×20×b×0.48d) / (0.87×415) = 3.456×0.48bd/361.05 = 0.00459bd
pt,bal = 100 × 0.00459 = 0.459% of bd (≈ 0.96% of bD for D/d ≈ 1.05)
6. Under-Reinforced, Balanced & Over-Reinforced
| Section Type | Condition | What Fails First | Failure Mode | IS 456 Permitted? |
|---|---|---|---|---|
| Under-reinforced | xu < xu,max Ast < Ast,bal pt < pt,bal | Steel yields first (εst reaches design yield strain) | Ductile — large deflections and visible cracking warn of impending failure | ✅ Yes — preferred |
| Balanced | xu = xu,max Ast = Ast,bal | Steel and concrete reach limits simultaneously | Transition between ductile and brittle | ✅ Yes — limiting case |
| Over-reinforced | xu > xu,max Ast > Ast,bal pt > pt,bal | Concrete crushes before steel yields | Brittle — sudden failure without warning | ❌ No — not permitted |
Why does more steel make the section more brittle? Adding more tension steel shifts the neutral axis deeper — more concrete area is needed in compression to balance the larger tension force. The deeper the neutral axis, the less strain the tension steel can undergo before the concrete at the top reaches its crushing strain. When xu is very large, the concrete crushes while the steel strain is still below yield — brittle failure. IS 456 prevents this by capping xu at xu,max.
7. Design Procedure — Finding Ast
Given: Design bending moment Mu, material grades (fck, fy), and either the section dimensions (b, d) or the breadth b with d to be determined.
Step 1 — Check if singly reinforced is adequate:
If section dimensions are given: compare Mu with Mu,lim = Ru,lim × bd².
- If Mu ≤ Mu,lim → singly reinforced section is adequate.
- If Mu > Mu,lim → singly reinforced is not adequate → use doubly reinforced or increase depth.
Step 2 — If d is unknown, find d from Mu,lim:
Set Mu = Mu,lim = Ru,lim × bd² → solve for d.
Choose a practical d (round up to standard value), then find Ast.
Step 3 — Find Ast from the design moment Mu:
Method 1 — Using the IS 456 Quadratic Formula
Mu = 0.87 fy Ast d [1 − (fy Ast)/(fck bd)]
Let p = Ast/(bd). Rearranging:
fyp² − fckp + Mufck/(0.87fybd²) = 0
Solve this quadratic in p = Ast/bd for Ast.
Take the smaller root (under-reinforced solution — the larger root is the over-reinforced solution which is not permitted).
Method 2 — Using the NA Depth (Two-Step Approach) ⭐ Preferred for GATE
Step A: Express Mu = 0.36 fck b xu (d − 0.42 xu)
Solve this quadratic in xu:
0.1512 fck b xu² − 0.36 fck b d xu + Mu = 0
xu = [0.36fckbd − √((0.36fckbd)² − 4×0.1512fckb×Mu)] / (2×0.1512fckb)
Check xu ≤ xu,max.
Step B: Find Ast from force equilibrium:
Ast = 0.36 fck b xu / (0.87 fy)
Step 4 — Select bar arrangement: Choose the number and diameter of bars such that the total area ≥ Ast required. Check spacing requirements (clear spacing ≥ max(φ, 25 mm, aggregate size + 5 mm)) and cover.
Step 5 — Check minimum and maximum steel:
- Ast,min = 0.85bd/fy (IS 456 Cl. 26.5.1.1)
- Ast,max = 0.04bD
8. Analysis Procedure — Finding Mu
Given: Section dimensions (b, d or D), steel area Ast, material grades.
- Find xu: xu = 0.87 fy Ast / (0.36 fck b)
- Check xu vs xu,max:
- If xu ≤ xu,max: proceed with xu as calculated (under-reinforced)
- If xu > xu,max: section is over-reinforced — use xu = xu,max for moment calculation (IS 456 limits this)
- Calculate Mu:
- If under-reinforced: Mu = 0.87 fy Ast (d − 0.42 xu)
- If over-reinforced: Mu = Mu,lim = 0.36 fck b xu,max (d − 0.42 xu,max)
9. Mu,lim Values — All Common Grade Combinations
Pre-Computed Ru,lim Values (Mu,lim = Ru,lim × bd² in N·mm)
| Steel Grade | M20 (fck=20) | M25 (fck=25) | M30 (fck=30) | M35 (fck=35) |
|---|---|---|---|---|
| Fe 250 (xu,max/d = 0.53) | 2.98 | 3.73 | 4.47 | 5.22 |
| Fe 415 (xu,max/d = 0.48) | 2.76 | 3.45 | 4.14 | 4.82 |
| Fe 500 (xu,max/d = 0.46) | 2.66 | 3.33 | 3.99 | 4.66 |
Units of Ru,lim: N/mm² (gives Mu,lim in N·mm when b and d are in mm)
To get Mu,lim in kN·m: Mu,lim (kN·m) = Ru,lim × b × d² × 10⁻⁶ (b, d in mm)
10. Worked Example 1 — Analysis (Find Mu)
Problem: A singly reinforced rectangular beam has b = 250 mm, d = 450 mm. Steel: 3 bars of 16 mm diameter (Ast = 603 mm²). fck = 20 N/mm², fy = 415 N/mm². Find the ultimate moment of resistance Mu.
Step 1 — Neutral Axis Depth xu
xu = 0.87 fy Ast / (0.36 fck b)
= (0.87 × 415 × 603) / (0.36 × 20 × 250)
= 217,614.45 / 1800
xu = 120.9 mm
Step 2 — Check Section Type
xu,max = 0.48 × d = 0.48 × 450 = 216 mm
xu = 120.9 mm < xu,max = 216 mm
→ Under-reinforced section ✓ (steel yields first — acceptable)
Step 3 — Moment of Resistance Mu
Mu = 0.87 fy Ast (d − 0.42 xu)
= 0.87 × 415 × 603 × (450 − 0.42 × 120.9)
= 217,614.45 × (450 − 50.78)
= 217,614.45 × 399.22
= 86,875,840 N·mm
Mu = 86.88 kN·m
Verification using C formula:
Mu = 0.36 × 20 × 250 × 120.9 × (450 − 0.42 × 120.9)
= 1800 × 120.9 × 399.22 = 217,620 × 399.22 = 86,878,000 N·mm ≈ 86.88 kN·m ✓
11. Worked Example 2 — Design (Find b, d and Ast)
Problem: Design a singly reinforced rectangular beam to carry a factored bending moment Mu = 120 kN·m. Use fck = 20 N/mm², fy = 415 N/mm². Assume b = 230 mm. Find the required effective depth d and area of steel Ast.
Step 1 — Find Effective Depth d
For the section to work as singly reinforced: Mu ≤ Mu,lim = Ru,lim × bd²
Setting Mu = Mu,lim (designing as balanced section for minimum d):
120 × 10⁶ = 2.76 × 230 × d²
d² = 120 × 10⁶ / (2.76 × 230) = 120,000,000 / 634.8 = 189,038
d = √189,038 = 434.8 mm → adopt d = 450 mm (round up to practical value)
Overall depth D = d + effective cover. Assuming effective cover = 50 mm: D = 450 + 50 = 500 mm.
Step 2 — Check Mu,lim for Adopted Section
Mu,lim = 2.76 × 230 × 450² = 2.76 × 230 × 202,500 = 128,547,000 N·mm = 128.55 kN·m
Mu = 120 kN·m < Mu,lim = 128.55 kN·m ✓ → Singly reinforced section is adequate.
Step 3 — Find Neutral Axis Depth xu
From Mu = 0.36 fck b xu (d − 0.42xu):
120 × 10⁶ = 0.36 × 20 × 230 × xu × (450 − 0.42xu)
120 × 10⁶ = 1656 xu (450 − 0.42xu)
120 × 10⁶ = 745,200 xu − 695.52 xu²
695.52 xu² − 745,200 xu + 120,000,000 = 0
Dividing by 695.52:
xu² − 1071.4 xu + 172,527 = 0
xu = [1071.4 − √(1071.4² − 4 × 172,527)] / 2
= [1071.4 − √(1,147,897.96 − 690,108)] / 2
= [1071.4 − √457,789.96] / 2
= [1071.4 − 676.6] / 2 = 394.8/2 = 197.4 mm
Wait — check: xu,max = 0.48 × 450 = 216 mm. xu = 197.4 < 216 ✓ Under-reinforced.
(Take the smaller root: [1071.4 − 676.6]/2 = 197.4 mm — this is correct. The larger root would be over-reinforced.)
Step 4 — Find Ast
Ast = 0.36 fck b xu / (0.87 fy)
= (0.36 × 20 × 230 × 197.4) / (0.87 × 415)
= (1656 × 197.4) / 361.05
= 326,894.4 / 361.05
Ast = 904.9 mm² ≈ 905 mm²
Bar selection: Provide 3 bars of 20 mm dia → Ast = 3 × 314.16 = 942.5 mm² > 905 mm² ✓
Or: 4 bars of 18 mm dia → Ast = 4 × 254.5 = 1018 mm² ✓
Step 5 — Check Minimum Steel
Ast,min = 0.85 bd / fy = 0.85 × 230 × 450 / 415 = 87,750 / 415 = 211.4 mm²
Ast,provided = 942.5 mm² > 211.4 mm² ✓
Final design: b = 230 mm, D = 500 mm, d = 450 mm, 3–20 mm dia bars (Ast = 942.5 mm²)
12. Worked Example 3 — Checking Adequacy of Given Section
Problem: A simply supported beam of span 5 m carries a dead load of 15 kN/m and live load of 10 kN/m (both including self-weight). The beam has b = 200 mm, D = 450 mm, d = 400 mm, and 2 bars of 20 mm dia (Ast = 628.3 mm²). fck = 25 N/mm², fy = 415 N/mm². Check if the section is adequate.
Step 1 — Design Bending Moment
Factored load wu = 1.5 × (15 + 10) = 1.5 × 25 = 37.5 kN/m
Mu = wuL²/8 = 37.5 × 25/8 = 117.19 kN·m
Step 2 — Section Capacity Mu,provided
xu = 0.87 × 415 × 628.3 / (0.36 × 25 × 200) = 226,700 / 1800 = 125.9 mm
xu,max = 0.48 × 400 = 192 mm
xu = 125.9 mm < 192 mm → Under-reinforced ✓
Mu,provided = 0.87 × 415 × 628.3 × (400 − 0.42 × 125.9)
= 226,700 × (400 − 52.88)
= 226,700 × 347.12
= 78,671,704 N·mm = 78.67 kN·m
Step 3 — Verdict
Mu,required = 117.19 kN·m > Mu,provided = 78.67 kN·m
The section is INADEQUATE. The beam cannot carry the applied loads.
Check if Mu,lim for this section would help: Mu,lim = 3.45 × 200 × 400² = 3.45 × 32,000,000 = 110.4 × 10⁶ N·mm = 110.4 kN·m
Even the balanced section capacity (110.4 kN·m) < required (117.19 kN·m) — a singly reinforced section of these dimensions cannot carry the load. Either increase depth or use doubly reinforced beam.
13. Worked Example 4 — GATE-Style Problem
Problem (GATE-style): The limiting moment of resistance of a singly reinforced rectangular beam section with b = 300 mm, d = 500 mm using M25 concrete and Fe 415 steel is (in kN·m):
Solution
Using Ru,lim for Fe 415, M25 = 3.45 N/mm²
Mu,lim = Ru,lim × b × d²
= 3.45 × 300 × 500²
= 3.45 × 300 × 250,000
= 3.45 × 75,000,000
= 258,750,000 N·mm
= 258.75 kN·m ≈ 259 kN·m
This type of problem is solvable in under 30 seconds once Ru,lim values are memorised — making it ideal for GATE time management.
14. Serviceability — Deflection Control
In addition to the strength (collapse) limit state, IS 456 requires that beams satisfy the serviceability limit state for deflection. Rather than computing actual deflections (which is complex for RCC members due to cracking and creep), IS 456 uses a simplified span-to-effective-depth ratio check.
IS 456 Span-to-Effective-Depth Ratio (Cl. 23.2)
Basic span/d ratios (for fy = 415 N/mm², pt ≈ 0.5%):
| Support Condition | Basic span/d Ratio |
|---|---|
| Simply supported beam | 20 |
| Continuous beam | 26 |
| Cantilever beam | 7 |
These basic ratios are modified by two factors:
Modification factor for tension steel (Mt): From IS 456 Fig. 4 — increases span/d for lower steel stress (under-stressed sections). Typically 1.0 to 2.0.
Modification factor for compression steel (Mc): From IS 456 Fig. 5 — increases span/d when compression steel is present. Typically 1.0 to 1.5.
Allowable span/d = Basic ratio × Mt × Mc
Deflection check: L/dprovided ≤ Allowable span/d
15. Common Mistakes Students Make
- Using overall depth D instead of effective depth d: All IS 456 LSM formulas for beams use the effective depth d — the distance from the compression face to the centroid of the tension steel. Using the overall depth D in the formula Mu = 0.87fyAst(D − 0.42xu) overestimates the moment capacity. Always check: does the problem give d directly, or do you need to calculate d from D minus the effective cover?
- Forgetting to check xu vs xu,max in analysis problems: In an analysis problem (given Ast, find Mu), always compute xu first and compare with xu,max. If xu > xu,max, the section is over-reinforced and Mu = Mu,lim, not 0.87fyAst(d − 0.42xu). Using the over-reinforced xu in the T formula significantly overestimates the moment capacity.
- Taking the wrong root in the quadratic for xu: The quadratic for xu in design problems always gives two roots. The smaller root corresponds to the under-reinforced (acceptable) solution. The larger root corresponds to the over-reinforced solution which is not permitted. Always take the smaller (physically meaningful) root.
- Applying the load factor after computing Mu,lim: Mu,lim and Mu in IS 456 are already at the ultimate level — they already incorporate the material partial safety factors (0.36fck and 0.87fy). The factored moment from loading (1.5 × working moment) is compared directly against Mu,lim. Do not multiply Mu,lim by 1.5 again — this double-counts the factor.
- Confusing pt = Ast/bd with Ast/bD: The steel percentage pt used in IS 456 design is 100Ast/(bd) where d is the effective depth. Some IS 456 tables (like the deflection modification factor chart) use percentage based on bd. Using bD instead of bd changes the percentage by the ratio D/d (typically 1.05 to 1.15), which is a non-trivial error for interpolation in IS 456 tables.
16. Frequently Asked Questions
Why is the lever arm (d − 0.42xu) and not (d − xu/2)?
The factor 0.42 comes from the IS 456 equivalent rectangular stress block. In a linear (triangular) stress distribution (as in WSM), the centroid of the triangular block is at x/3 from the top, giving lever arm = d − x/3. In LSM, IS 456 uses an equivalent rectangular stress block of intensity 0.36fck over a depth of 0.42xu. The centroid of this rectangular block is at 0.42xu/2 = 0.21xu from the top... but IS 456 writes the lever arm as d − 0.42xu, meaning it places the centroid at 0.42xu from the compression face. This is because the 0.42 factor in IS 456 already accounts for the combined effect of the parabolic portion and the rectangular portion of the actual stress-strain curve, placing the centroid of the resultant compressive force at 0.42xu from the extreme compression fibre. This is a standard IS 456 result — use 0.42 without question in all IS 456 calculations.
What is the difference between Mu and Mu,lim?
Mu is the actual moment of resistance of a specific section — it depends on the actual amount of steel provided (Ast) and the resulting neutral axis depth xu. Mu,lim is the limiting (maximum) moment of resistance of a singly reinforced section of given b and d — it corresponds to the balanced condition where xu = xu,max. For any under-reinforced section, Mu < Mu,lim. Adding more steel increases Mu until it reaches Mu,lim at the balanced condition. Adding steel beyond balanced increases xu beyond xu,max — this is not permitted, so Mu stays at Mu,lim.
Can I use the formula Mu,lim = 2.76 bd² directly for all problems?
The value 2.76 bd² applies specifically to Fe 415 steel with M20 concrete. If the steel grade or concrete grade is different, use the appropriate Ru,lim from the table. The formula Mu,lim = Ru,lim × bd² is always valid — only the coefficient Ru,lim changes with the material grades. For GATE CE problems, if the grades are not specified, Fe 415 and M20 are the standard assumed grades. Always check the problem statement before applying any pre-computed coefficient.
What happens to the moment capacity if the concrete grade is increased while keeping everything else the same?
Increasing fck while keeping the same b, d, and Ast has two effects. First, it increases the compressive capacity of the concrete, which reduces the required neutral axis depth xu for the same tensile force — the section becomes more under-reinforced. Second, the higher fck shifts the neutral axis upward, increasing the lever arm (d − 0.42xu), which slightly increases Mu. In practice, for typical under-reinforced sections, the moment capacity is not very sensitive to the concrete grade — it is dominated by the steel area and yield strength. This is why increasing concrete grade is not an efficient way to increase moment capacity; increasing steel area or effective depth is much more effective.