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Principal MI and axis of composite section

Short answer

Composite-area method: centroid (500, 100) mm; I_x = 4.027×10^10, I_y = 5.627×10^10, I_xy = –3.600×10^10 mm^4. Principal moments: I_max = 8.514×10^10 mm^4, I_min = 1.139×10^10 mm^4. Principal axes through centroid at 51.26° (I_max) and –38.74° (I_min) from +x axis.

Determine the principle moment of inertia and orientation of principle axis for the section shown in the figure below about centroid, all dimensions are in mm. [Figure: composite section made of a vertical triangle at the top left (height 600, with a 600 horizontal dimension), a horizontal rectangular strip of length 1000 and 200 thick, and a lower right triangle with horizontal dimension 600 and height 600; overall dimensions: 600, 1000, 600 horizontal at the bottom, 200 and 600 vertical on the right.]

Dimensions and assumptions (read from the figure):

  • Dimensions in mm. Strip: 1000 × 200 (x 0 to 1000, y 0 to 200). Upper-left right triangle: vertices (0,200), (600,200), (0,800). Lower-right right triangle: vertices (1000,0), (400,0), (1000,−600).

Properties of the parts (x, y measured from the reference origin; IGI_G about the part's own centroid; area in mm2mm^2, I in mm4mm^4)

PartSignAxˉ\bar xyˉ\bar yIx,GI_{x,G}Iy,GI_{y,G}Ixy,GI_{xy,G}
Strip 1000×200+2.000×1052.000\times10^{5}500.0100.06.667×1086.667\times10^{8}1.667×10101.667\times10^{10}00
Upper triangle+1.800×1051.800\times10^{5}200.0400.03.600×1093.600\times10^{9}3.600×1093.600\times10^{9}−1.800×109-1.800\times10^{9}
Lower triangle+1.800×1051.800\times10^{5}800.0-200.03.600×1093.600\times10^{9}3.600×1093.600\times10^{9}−1.800×109-1.800\times10^{9}

Centroid

A=∑Ai=5.600×105 mm2Xˉ=∑AixiA=2.800×1085.600×105=500.0 mmYˉ=∑AiyiA=5.600×1075.600×105=100.0 mm\begin{aligned} A &= \sum A_i = 5.600\times10^{5}\ \text{mm}^2 \\ \bar X &= \frac{\sum A_i x_i}{A} = \frac{2.800\times10^{8}}{5.600\times10^{5}} = 500.0\ \text{mm} \\ \bar Y &= \frac{\sum A_i y_i}{A} = \frac{5.600\times10^{7}}{5.600\times10^{5}} = 100.0\ \text{mm} \end{aligned}

Moments and product of inertia about the centroidal axes

With dx=xi−Xˉd_x = x_i-\bar X, dy=yi−Yˉd_y = y_i-\bar Y and the parallel-axis theorems Ix=Ix,G+Ady2I_x = I_{x,G}+Ad_y^2, Iy=Iy,G+Adx2I_y = I_{y,G}+Ad_x^2, Ixy=Ixy,G+AdxdyI_{xy} = I_{xy,G}+Ad_xd_y:

PartIx,G+Ady2I_{x,G}+A d_y^2Iy,G+Adx2I_{y,G}+A d_x^2Ixy,G+AdxdyI_{xy,G}+A d_x d_y
Strip 1000×200 (+)6.667×1086.667\times10^{8}1.667×10101.667\times10^{10}00
Upper triangle (+)1.980×10101.980\times10^{10}1.980×10101.980\times10^{10}−1.800×1010-1.800\times10^{10}
Lower triangle (+)1.980×10101.980\times10^{10}1.980×10101.980\times10^{10}−1.800×1010-1.800\times10^{10}
Total about centroid4.027×10104.027\times10^{10}5.627×10105.627\times10^{10}−3.600×1010-3.600\times10^{10}

Principal moments of inertia and principal axes

Imax,min=Ix+Iy2±(Ix−Iy2)2+Ixy2=4.827×1010±3.688×1010Imax=8.514×1010 mm4,Imin=1.139×1010 mm4\begin{aligned} I_{max,min} &= \frac{I_x+I_y}{2}\pm\sqrt{\left(\frac{I_x-I_y}{2}\right)^2+I_{xy}^2} \\ &= 4.827\times10^{10}\pm3.688\times10^{10} \\ I_{max} &= 8.514\times10^{10}\ \text{mm}^4,\qquad I_{min} = 1.139\times10^{10}\ \text{mm}^4 \end{aligned}

Orientation: tan⁡2θp=−2IxyIx−Iy=7.200×1010−1.600×1010\tan 2\theta_p = \dfrac{-2I_{xy}}{I_x-I_y} = \dfrac{7.200\times10^{10}}{-1.600\times10^{10}}, so 2θp=102.53∘2\theta_p = 102.53^\circ (and −77.47∘-77.47^\circ).

  • The axis of ImaxI_{max} makes 51.26° with the +x axis (anticlockwise positive); the axis of IminI_{min} is at -38.74° (perpendicular), both passing through the centroid (500.0, 100.0) measured from the reference origin.

Answer: Imax=8.514×1010 mm4I_{max} = 8.514\times10^{10}\ \text{mm}^4, Imin=1.139×1010 mm4I_{min} = 1.139\times10^{10}\ \text{mm}^4; principal axes through the centroid at 51.26° (for ImaxI_{max}) and -38.74° (for IminI_{min}) from the +x axis.

✓ Answer checked by Claude Opus 5.5 (high effort)

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