Answer:
The correct answer is D 
 /
 = 1.5
Step-by-step explanation:
In this exercise the moment of inertia equation should be used 
 I = ∫ r² dm 
In addition to the parallel axis theorem 
 I = 
 + M D² 
Where 
 is the moment of the center of mass, M is the total mass of the body and D the distance from this point to the axis of interest 
Let's apply these relationships to our problem, the center of mass of a uniform rod coincides with its geometric center, in this case the rod is 1 m long, so the center of mass is in 
 L = 100.00 cm (1m / 100 cm) = 1.0000 m 
 
 = 50 cm = 0.50 m 
Let's calculate the moment of inertia for this point, suppose the rod is on the x-axis and use the concept of linear density 
 λ = M / L = dm / dx 
 dm = λ dx 
Let's replace in the moment of inertia equation 
 I = ∫ x² ( λ dx) 
We integrate 
 I = λ x³ / 3 
We evaluate between the lower limits x = -L/2 to the upper limit x = L/2
 I = λ/3 [(L/2)³ - (-L/2)³] = lam/3 [L³/8 - (-L³ / 8)] 
 I = λ/3 L³/4 
 I = 1/12 λ L³ 
Let's replace the linear density with its value 
 I = 1/12 (M/L) L³ 
 I = 1/12 M L² 
Let's calculate with the given values 
 I = 1/12 M 1² 
 I = 1/12 M 
This point is the center of mass of the rod 
 Icm = I = 1/12 M = 8.333 10-2 M 
 
Now let's use the parallel axis theorem to calculate the moment of resection of the new axis, which is 0.30 m from one end, in this case the distance is 
 D = 
 - x 
 D = 0.50 - 0.30 
 D = 0.20 m 
Let's calculate 
 
 =
 + M D² 
 
 = 1/12 M + M 0.202 
 
 = M (1/12 + 0.04) 
 
 = M 0.123 
 
To find the relationship between the two moments of inertia, divide the quantities 
 
 / 
 = M 0.123 / (M 8.3 10-2) 
 
 /
 = 1.48 
 
The correct answer is d 1.5