Concept:The sum involves an integral with ∣sinπx∣ which is periodic with period 1.By substitution and periodicity, the integral simplifies to a sum of odd numbers, yielding r2/π.Explanation:Define Jr=∫0rx∣sinπx∣dx.We need I=∑r=120πJr.Substitute t=πx, so dx=dt/π.Then Jr=∫0πrπt∣sint∣πdt=π21∫0πrt∣sint∣dt.Since ∣sint∣ has period π, break the integral into intervals of length π: ∫0πrt∣sint∣dt=∑k=0r−1∫kπ(k+1)πt∣sint∣dt.In (0,π), ∣sint∣=sint; in (π,2π), ∣sint∣=−sint; pattern alternates with sign (−1)k.Thus ∫0πrt∣sint∣dt=∑k=0r−1(−1)k∫kπ(k+1)πtsintdt.Integrate ∫tsintdt=−tcost+sint (by parts).Evaluate at limits: for interval kπ to (k+1)π, let F(t)=−tcost+sint.F((k+1)π)−F(kπ)=[−(k+1)π(−1)k+1+0]−[−kπ(−1)k+0]=(k+1)π(−1)k−kπ(−1)k+1? Wait carefully: cos(kπ)=(−1)k, sin(kπ)=0. So:F((k+1)π)=−(k+1)π(−1)k+1=(k+1)π(−1)k (since −(−1)k+1=(−1)k).F(kπ)=−kπ(−1)k=−kπ(−1)k.Difference = (k+1)π(−1)k+kπ(−1)k=(2k+1)π(−1)k.But in the alternating sum, we have (−1)k times this difference, so term becomes (2k+1)π.Thus ∫0πrt∣sint∣dt=∑k=0r−1(2k+1)π=π⋅(sum of first r odd numbers)=πr2.Therefore Jr=π21⋅πr2=πr2.Now I=∑r=120π⋅πr2=∑r=120r=220×21=210.Answer:210 (option A).