Question 20.11: A baseball bat has a uniform handle AB of length 0.36 m and ...

A baseball bat has a uniform handle AB of length 0.36 m and mass M_{1} = 0.136 kg. The remainder of the bat is modelled as a thin rod BC of length 0.7 m and mass per unit length 1.43(x² + x + 0.25) kg m^{-1}, where x is the distance from B. Assuming the handle can also be modelled as a thin rod, find
i)    the mass M kg of the bat
ii)   the distance of its centre of mass, G, from B
iii)  its moment of inertia about a perpendicular axis through B
iv)  its moment of inertia about a perpendicular axis through the end A.

fig 20.25
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figure 20.26 shows the essential features of the bat.

i) The mass of an element of BC of length δx is 1.43(x² + x + 0.25)δx kg

⇒      mass of BC = \int_{0}^{0.7}{1.43(x² + x + 0.25)dx kg}

= \left[1.43\left(\frac{x^{3}}{3} + \frac{x^{2}}{2} + 0.25x\right)\right]^{0.7}_{0} kg

= 0.764 kg

⇒        Total mass M = 0.764 + 0.136 = 0.900 kg (to 3 significant figures).

ii) To find the distance, \bar{x}, of G from B, take moments about an axis through B. Then

\left(\sum{δm}\right) \bar{x} = \sum{(δmx)}      (summed for all particles of the bat).

For AB       \sum{(δmx)} = – M_{1} × \frac{1}{2}AB

= – 0.136 × 0.18

= – 0.0245

and for BC ∑ (δmx) = ∑ 1.43 (x² + x + 0.25)x δx.

In the limit as δx → 0, this becomes

\int_{0}^{0.7}{1.43(x² + x + 0.25)x dx}

= \int_{0}^{0.7}{1.43(x³ + x² + 0.25x) dx}

= 1.43\left[\frac{x^{4}}{4}  +  \frac{x^{3}}{3}  +  0.25\frac{x^{2}}{2}\right]^{0.7}_{0}

= 0.3369.

Combining AB and BC gives

0.9 \bar{x} = – 0.0245  +  0.3369

⇒      0.9 \bar{x} = 0.3124

\bar{x} = 0.347.

The centre of mass is about 35 cm from B.

iii) The moment of inertia, I_{1}, of the uniform rod AB about a perpendicular axis through its centre is \frac{1}{3}M_{1}(0.18)². So, by the parallel axes theorem, its moment of inertia about the end B is

I_{1} = \frac{1}{3}M_{1}(0.18)²  +  M_{1}(0.18)²

= \frac{4}{3}(0.136)(0.18)²

= 0.0059 kg m².

The moment of inertia, I_{2}, of the part BC about the axis through B is

I_{2} = \underset{δx-0}{lim} (\sum{\delta mx^{2}})

= \int_{0}^{0.7}{1.43(x² + x + 0.25)x² dx}

= \int_{0}^{0.7}{1.43(x^{4} + x³ + 0.25x²) dx}

= 1.43\left[\frac{x^{5}}{5}  +  \frac{x^{4}}{4}  +  0.25\frac{x^{3}}{3}\right]^{0.7}_{0}

= 0.1748.

Hence:              I_{1}  +  I_{2} = 0.1807.

The moment of inertia of the bat about a perpendicular axis through B is about 0.18 kg m².

iv) By the parallel axes theorem,

  I_{B} = I_{G} + M(BG)²

and               I_{A} = I_{G} + M(AG)²

⇒                  I_{A} = I_{B}  –  M(BG)²  +  M(AG)²

⇒                  I_{A} = I_{B}  +  M(AG²  –  BG²)

= 0.1807 + 0.9(0.3795)

= 0.5222

The moment of inertia about the end, A, is about 0.52 kg m².

fig 20.26
fig 20.27

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