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Moment of Inertia Parallel Axis Theorem

Statics · FE Reference Handbook section

Statics
5 formulas
10 exam-style examples
~55 min
All Statics lectures

Handbook notes for this section

Definitions and conditions exactly as the handbook states them.

  • The moment of inertia of an area about any axis is defined as the moment of inertia of the area about a parallel centroidal axis
  • plus a term equal to the area multiplied by the square of the perpendicular distance d from the centroidal axis to the axis in

Core formulas for this FE topic

Definitions, applicability, units, assumptions and worked examples for each relation.

Worked exam-style examples

The four ways this section is written on the real exam — thoughts first, then equations, then substitution.

Example 1
Moment of inertia of a T-section

A T-section has a 200 mm × 40 mm flange on top of a 40 mm × 260 mm web. Find the centroid from the bottom and I about the centroidal axis.

Given

  • Flange 200 × 40 mm at top

  • Web 40 × 260 mm below it

Find

ȳ from bottom and I_x

Start with the thinking

  • Take areas and their own centroids first, then use the parallel-axis theorem.
  • Measure all distances from a single datum — the bottom fibre.

Step-by-step solution

  1. Areas

    Aweb=40(260)=10,400mm2andAflange=200(40)=8,000mm2A_web = 40(260) = 10,400 mm^{2} and A_flange = 200(40) = 8,000 mm^{2}
  2. Local centroids

    yweb=130mmandyflange=260+20=280mmy_web = 130 mm and y_flange = 260 + 20 = 280 mm
  3. Centroid

    yˉ=[10,400(130)+8,000(280)]/18,400=(1,352,000+2,240,000)/18,400=195.2mmȳ = [10,400(130) + 8,000(280)]/18,400 = (1,352,000 + 2,240,000)/18,400 = 195.2 mm
  4. Web term

    I=40(260)3/12+10,400(195.2−130)2=58.6×106+44.2×106=102.8×106mm4I = 40(260)^{3}/12 + 10,400(195.2 - 130)^{2} = 58.6\times10^{6} + 44.2\times10^{6} = 102.8\times10^{6} mm^{4}
  5. Flange term

    I=200(40)3/12+8,000(280−195.2)2=1.07×106+57.5×106=58.6×106mm4I = 200(40)^{3}/12 + 8,000(280 - 195.2)^{2} = 1.07\times10^{6} + 57.5\times10^{6} = 58.6\times10^{6} mm^{4}
  6. Total

    Ix=102.8×106+58.6×106=161×106mm4I_x = 102.8\times10^{6} + 58.6\times10^{6} = 161\times10^{6} mm^{4}
Answer:
yˉ=195mmfromthebottom,Ix≈161×106mm4ȳ = 195 mm from the bottom, I_x \approx 161 \times 10^{6} mm^{4}

Why the other options are there

  • I = 59.7 × 10⁶ mm⁴ (parallel-axis terms omitted)
  • ȳ = 150 mm (areas averaged, not weighted)

Reference: FE Reference Handbook — Statics — Centroids and moments of inertia

Example 2
Moment of a force — solve for moment — Moment of Inertia Parallel Axis Theorem

A statics problem uses Moment of a force. Given force (F) = 1,232 lb; moment arm (d) = 5.0000 ft, determine the moment (M) in lb·ft.

Given

  • force(F)=1,232lbforce (F) = 1,232 lb
  • momentarm(d)=5.0000ftmoment arm (d) = 5.0000 ft

Find

moment (M), in lb·ft

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force.
  • Everything except M is given, so isolate M symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • Statics items reward recognising the unknown before touching a calculator.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=F×dM = F \times d
  2. Step 2 — Rearrange the relation so that M stands alone on the left-hand side.

  3. Step 3

    Listthegivens:force(F)=1,232lb,momentarm(d)=5.0000ftList the givens: force (F) = 1,232 lb, moment arm (d) = 5.0000 ft
  4. Step 4 — Substitute the given values into the rearranged relation.

  5. Step 5 — Evaluate:

    M=6160 lb⋅ftM = 6160\ \text{lb·ft}
  6. Step 6 — Check: returning M = 6,160 lb·ft to

    M=F×dM = F \times d

    reproduces the given quantities, and both sides carry the same units.

Answer:
M=6160 lb⋅ftM = 6160\ \text{lb·ft}

Why the other options are there

  • 12,320 — kept a factor of two that cancels in the correct rearrangement.
  • 3,080 — dropped that same factor in the other direction.
  • 6,776 — rounded an intermediate value before the final step.

Reference: FE Reference Handbook — Statics → Moment of Inertia Parallel Axis Theorem

Example 3
Moment of a force about a point — solve for moment — Moment of Inertia Parallel Axis Theorem (2)

a cantilevered sign arm Given force (F) = 3,441 N; perpendicular distance (d) = 0.7000 m, determine the moment (M) in N\cdot m.

Given

  • force(F)=3,441Nforce (F) = 3,441 N
  • perpendiculardistance(d)=0.7000mperpendicular distance (d) = 0.7000 m

Find

moment (M), in N\cdot m

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force about a point.
  • Everything except M is given, so isolate M symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • A force acting at a perpendicular distance d produces a moment.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=FdM = F d
  2. Step 2 — Rearrange symbolically for M:

    M=M=FdM = M = F d
  3. Step 3

    Listthegivens:force(F)=3,441N,perpendiculardistance(d)=0.7000mList the givens: force (F) = 3,441 N, perpendicular distance (d) = 0.7000 m
  4. Step 4 — Substitute the given values:

    M=M=34410.7000M = M = 3441 0.7000
  5. Step 5 — Evaluate:

    M=2409 N\cdotmM = 2409\ \text{N\cdot m}
  6. Step 6 — Check: returning M = 2,409 N\cdot m to

    M=FdM = F d

    reproduces the given quantities, and both sides carry the same units.

Answer:
M=2409 N\cdotmM = 2409\ \text{N\cdot m}

Why the other options are there

  • 4,817 — kept a factor of two that cancels in the correct rearrangement.
  • 1,204 — dropped that same factor in the other direction.
  • 2,649 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics (Moments)

Example 4
Rectangular moment of inertia — solve for moment of inertia — Moment of Inertia Parallel Axis Theorem (3)

A rectangular concrete section's moment of inertia is used in a stiffness calculation. Given width (b) = 8.5000 in; height (h) = 15.4000 in, determine the moment of inertia (I) in in^4.

Given

  • width(b)=8.5000inwidth (b) = 8.5000 in
  • height(h)=15.4000inheight (h) = 15.4000 in

Find

moment of inertia (I), in in^4

Start with the thinking

  • The governing relation printed in this handbook section is Rectangular moment of inertia.
  • Everything except I is given, so isolate I symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • The moment of inertia of a rectangular cross section about its centroidal axis governs bending stiffness.
Rectangular sectioncentroidal axisb = 6h = 12

Figure 4 — schematic for Rectangular moment of inertia — solve for moment of inertia — Moment of Inertia Parallel Axis Theorem (3)

Step-by-step solution

  1. Step 1 — State the governing relation:

    I=bh312I = \dfrac{b h^3}{12}
  2. Step 2 — Rearrange symbolically for I:

    I=bh312I = \dfrac{b h^3}{12}
  3. Step 3

    Listthegivens:width(b)=8.5000in,height(h)=15.4000inList the givens: width (b) = 8.5000 in, height (h) = 15.4000 in
  4. Step 4 — Substitute the given values:

    I=8.500015.4000312I = \dfrac{8.5000 15.4000^3}{12}
  5. Step 5 — Evaluate:

    I = 2587\ \text{in^4}
  6. Step 6 — Check: returning I = 2,587 in^4 to

    I=bh312I = \dfrac{b h^3}{12}

    reproduces the given quantities, and both sides carry the same units.

Answer:
I = 2587\ \text{in^4}

Why the other options are there

  • 5,174 — kept a factor of two that cancels in the correct rearrangement.
  • 1,294 — dropped that same factor in the other direction.
  • 2,846 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics: Moment of Inertia

Example 5
Moment of a force — solve for force — Moment of Inertia Parallel Axis Theorem (4)

A statics problem uses Moment of a force. Given moment arm (d) = 7.5000 ft; moment (M) = 16,502 lb·ft, determine the force (F) in lb.

Given

  • momentarm(d)=7.5000ftmoment arm (d) = 7.5000 ft
  • moment (M) = 16,502 lb·ft

Find

force (F), in lb

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force.
  • Everything except F is given, so isolate F symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • Statics items reward recognising the unknown before touching a calculator.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=F×dM = F \times d
  2. Step 2 — Rearrange the relation so that F stands alone on the left-hand side.

  3. Step 3 — List the givens: moment arm (d) = 7.5000 ft, moment (M) = 16,502 lb·ft.

  4. Step 4 — Substitute the given values into the rearranged relation.

  5. Step 5 — Evaluate:

    F=2200 lbF = 2200\ \text{lb}
  6. Step 6 — Check: returning F = 2,200 lb to

    M=F×dM = F \times d

    reproduces the given quantities, and both sides carry the same units.

Answer:
F=2200 lbF = 2200\ \text{lb}

Why the other options are there

  • 4,401 — kept a factor of two that cancels in the correct rearrangement.
  • 1,100 — dropped that same factor in the other direction.
  • 2,420 — rounded an intermediate value before the final step.

Reference: FE Reference Handbook — Statics → Moment of Inertia Parallel Axis Theorem

Example 6
Moment of a force about a point — solve for force — Moment of Inertia Parallel Axis Theorem (5)

a wrench applied to an anchor nut Given moment (M) = 4,687 N\cdot m; perpendicular distance (d) = 1.9000 m, determine the force (F) in N.

Given

  • moment(M)=4,687N⋅mmoment (M) = 4,687 N\cdot m
  • perpendiculardistance(d)=1.9000mperpendicular distance (d) = 1.9000 m

Find

force (F), in N

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force about a point.
  • Everything except F is given, so isolate F symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • A force acting at a perpendicular distance d produces a moment.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=FdM = F d
  2. Step 2 — Rearrange symbolically for F:

    F=F=MdF = F = \dfrac{M}{d}
  3. Step 3

    Listthegivens:moment(M)=4,687N⋅m,perpendiculardistance(d)=1.9000mList the givens: moment (M) = 4,687 N\cdot m, perpendicular distance (d) = 1.9000 m
  4. Step 4 — Substitute the given values:

    F=F=46871.9000F = F = \dfrac{4687}{1.9000}
  5. Step 5 — Evaluate:

    F=2467 NF = 2467\ \text{N}
  6. Step 6 — Check: returning F = 2,467 N to

    M=FdM = F d

    reproduces the given quantities, and both sides carry the same units.

Answer:
F=2467 NF = 2467\ \text{N}

Why the other options are there

  • 4,933 — kept a factor of two that cancels in the correct rearrangement.
  • 1,233 — dropped that same factor in the other direction.
  • 2,713 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics (Moments)

Example 7
Rectangular moment of inertia — solve for width — Moment of Inertia Parallel Axis Theorem (6)

A rectangular wood beam's moment of inertia is needed for a deflection check. Given height (h) = 11.0000 in; moment of inertia (I) = 11,078 in^4, determine the width (b) in in.

Given

  • height(h)=11.0000inheight (h) = 11.0000 in
  • momentofinertia(I)=11,078in4moment of inertia (I) = 11,078 in^4

Find

width (b), in in

Start with the thinking

  • The governing relation printed in this handbook section is Rectangular moment of inertia.
  • Everything except b is given, so isolate b symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • The moment of inertia of a rectangular cross section about its centroidal axis governs bending stiffness.
Rectangular sectioncentroidal axisb = 6h = 12

Figure 7 — schematic for Rectangular moment of inertia — solve for width — Moment of Inertia Parallel Axis Theorem (6)

Step-by-step solution

  1. Step 1 — State the governing relation:

    I=bh312I = \dfrac{b h^3}{12}
  2. Step 2 — Rearrange symbolically for b:

    b=12Ih3b = \dfrac{12 I}{h^3}
  3. Step 3

    Listthegivens:height(h)=11.0000in,momentofinertia(I)=11,078in4List the givens: height (h) = 11.0000 in, moment of inertia (I) = 11,078 in^4
  4. Step 4 — Substitute the given values:

    b=121107811.00003b = \dfrac{12 11078}{11.0000^3}
  5. Step 5 — Evaluate:

    b=99.8768 inb = 99.8768\ \text{in}
  6. Step 6 — Check: returning b = 99.8768 in to

    I=bh312I = \dfrac{b h^3}{12}

    reproduces the given quantities, and both sides carry the same units.

Answer:
b=99.8768 inb = 99.8768\ \text{in}

Why the other options are there

  • 199.8 — kept a factor of two that cancels in the correct rearrangement.
  • 49.9384 — dropped that same factor in the other direction.
  • 109.9 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics: Moment of Inertia

Example 8
Moment of a force — solve for moment arm — Moment of Inertia Parallel Axis Theorem (7)

A statics problem uses Moment of a force. Given force (F) = 819.0 lb; moment (M) = 8,453 lb·ft, determine the moment arm (d) in ft.

Given

  • force(F)=819.0lbforce (F) = 819.0 lb
  • moment (M) = 8,453 lb·ft

Find

moment arm (d), in ft

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force.
  • Everything except d is given, so isolate d symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • Statics items reward recognising the unknown before touching a calculator.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=F×dM = F \times d
  2. Step 2 — Rearrange the relation so that d stands alone on the left-hand side.

  3. Step 3 — List the givens: force (F) = 819.0 lb, moment (M) = 8,453 lb·ft.

  4. Step 4 — Substitute the given values into the rearranged relation.

  5. Step 5 — Evaluate:

    d=10.3211 ftd = 10.3211\ \text{ft}
  6. Step 6 — Check: returning d = 10.3211 ft to

    M=F×dM = F \times d

    reproduces the given quantities, and both sides carry the same units.

Answer:
d=10.3211 ftd = 10.3211\ \text{ft}

Why the other options are there

  • 20.6422 — kept a factor of two that cancels in the correct rearrangement.
  • 5.1606 — dropped that same factor in the other direction.
  • 11.3532 — rounded an intermediate value before the final step.

Reference: FE Reference Handbook — Statics → Moment of Inertia Parallel Axis Theorem

Example 9
Moment of a force about a point — solve for perpendicular distance — Moment of Inertia Parallel Axis Theorem (8)

a bracket bolted to a column flange Given moment (M) = 7,286 N\cdot m; force (F) = 1,936 N, determine the perpendicular distance (d) in m.

Given

  • moment(M)=7,286N⋅mmoment (M) = 7,286 N\cdot m
  • force(F)=1,936Nforce (F) = 1,936 N

Find

perpendicular distance (d), in m

Start with the thinking

  • The governing relation printed in this handbook section is Moment of a force about a point.
  • Everything except d is given, so isolate d symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • A force acting at a perpendicular distance d produces a moment.

Step-by-step solution

  1. Step 1 — State the governing relation:

    M=FdM = F d
  2. Step 2 — Rearrange symbolically for d:

    d=d=MFd = d = \dfrac{M}{F}
  3. Step 3

    Listthegivens:moment(M)=7,286N⋅m,force(F)=1,936NList the givens: moment (M) = 7,286 N\cdot m, force (F) = 1,936 N
  4. Step 4 — Substitute the given values:

    d=d=72861936d = d = \dfrac{7286}{1936}
  5. Step 5 — Evaluate:

    d=3.7627 md = 3.7627\ \text{m}
  6. Step 6 — Check: returning d = 3.7627 m to

    M=FdM = F d

    reproduces the given quantities, and both sides carry the same units.

Answer:
d=3.7627 md = 3.7627\ \text{m}

Why the other options are there

  • 7.5255 — kept a factor of two that cancels in the correct rearrangement.
  • 1.8814 — dropped that same factor in the other direction.
  • 4.1390 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics (Moments)

Example 10
Rectangular moment of inertia — solve for height — Moment of Inertia Parallel Axis Theorem (9)

A steel plate's moment of inertia about its centroidal axis is computed for buckling. Given width (b) = 10.9000 in; moment of inertia (I) = 13,423 in^4, determine the height (h) in in.

Given

  • width(b)=10.9000inwidth (b) = 10.9000 in
  • momentofinertia(I)=13,423in4moment of inertia (I) = 13,423 in^4

Find

height (h), in in

Start with the thinking

  • The governing relation printed in this handbook section is Rectangular moment of inertia.
  • Everything except h is given, so isolate h symbolically first — never rearrange after the numbers are in.
  • Tabulate each given with its unit and confirm the units are consistent with the relation before substituting.
  • The moment of inertia of a rectangular cross section about its centroidal axis governs bending stiffness.
Rectangular sectioncentroidal axisb = 6h = 12

Figure 10 — schematic for Rectangular moment of inertia — solve for height — Moment of Inertia Parallel Axis Theorem (9)

Step-by-step solution

  1. Step 1 — State the governing relation:

    I=bh312I = \dfrac{b h^3}{12}
  2. Step 2 — Rearrange symbolically for h:

    h=12Ib3h = \sqrt[3]{\dfrac{12 I}{b}}
  3. Step 3

    Listthegivens:width(b)=10.9000in,momentofinertia(I)=13,423in4List the givens: width (b) = 10.9000 in, moment of inertia (I) = 13,423 in^4
  4. Step 4 — Substitute the given values:

    h=121342310.90003h = \sqrt[3]{\dfrac{12 13423}{10.9000}}
  5. Step 5 — Evaluate:

    h=24.5396 inh = 24.5396\ \text{in}
  6. Step 6 — Check: returning h = 24.5396 in to

    I=bh312I = \dfrac{b h^3}{12}

    reproduces the given quantities, and both sides carry the same units.

Answer:
h=24.5396 inh = 24.5396\ \text{in}

Why the other options are there

  • 49.0793 — kept a factor of two that cancels in the correct rearrangement.
  • 12.2698 — dropped that same factor in the other direction.
  • 26.9936 — rounded an intermediate value before the final step.

Reference: FE Handbook — Statics: Moment of Inertia

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