Question
Question: A rigid body can be hinged about any point on the x-axis. When it is hinged such that the hinge is a...
A rigid body can be hinged about any point on the x-axis. When it is hinged such that the hinge is at x, the moment of inertia is given by I=2x2−12x+27. The x-coordinate of centre of mass is

x = 2
x = 0
a parabola
x = 1
a straight line
x=3
x=3
Solution
The moment of inertia of a rigid body about an axis is given by the parallel axis theorem:
I=ICM+Md2
where ICM is the moment of inertia about a parallel axis passing through the center of mass, M is the mass of the body, and d is the perpendicular distance between the two parallel axes.
In this problem, the hinge is at x, and let the x-coordinate of the center of mass be xCM. The distance d between the hinge and the center of mass is ∣x−xCM∣. So, d2=(x−xCM)2.
Substituting this into the parallel axis theorem: I=ICM+M(x−xCM)2 Expand the term (x−xCM)2: I=ICM+M(x2−2x⋅xCM+xCM2) Rearrange the terms to match the form of a quadratic equation in x: I=Mx2−(2MxCM)x+(ICM+MxCM2)
We are given the moment of inertia as: I=2x2−12x+27
Now, we compare the coefficients of the given equation with the expanded form from the parallel axis theorem:
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Comparing the coefficient of x2: From the general form: Coefficient of x2 is M. From the given equation: Coefficient of x2 is 2. Therefore, M=2.
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Comparing the coefficient of x: From the general form: Coefficient of x is −2MxCM. From the given equation: Coefficient of x is −12. Therefore, −2MxCM=−12. Substitute the value of M=2: −2(2)xCM=−12 −4xCM=−12 xCM=−4−12 xCM=3
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Comparing the constant term: From the general form: Constant term is (ICM+MxCM2). From the given equation: Constant term is 27. Therefore, ICM+MxCM2=27. Substitute the values of M=2 and xCM=3: ICM+2(3)2=27 ICM+2(9)=27 ICM+18=27 ICM=27−18 ICM=9
From the comparison, the x-coordinate of the center of mass is xCM=3.