We are tasked with evaluating the limit:
n→∞limn514+24+⋯+n4−n→∞limn513+23+⋯+n3
Instead of using tedious summation formulas, we utilize the
Riemann Sum identity, which acts as a bridge between discrete sums and continuous integration:
n→∞limn1r=1∑nf(nr)=∫01f(x)dx
Let the first term be
L1=limn→∞n5∑r=1nr4. To apply the identity, we rewrite the expression to isolate the
n1 factor:
L1=n→∞limn1r=1∑nn4r4=n→∞limn1r=1∑n(nr)4
By substituting
nr=x and
n1=dx, the summation transforms into a definite integral:
L1=∫01x4dx
Evaluating this integral yields:
L1=[5x5]01=51
Now, consider the second term
L2=limn→∞n5∑r=1nr3. We manipulate the denominator to reveal the Riemann structure:
L2=n→∞lim(n1⋅n41r=1∑nr3)=n→∞lim(n1⋅n1r=1∑n(nr)3)
The bracketed expression
n1∑r=1n(nr)3 converges to
∫01x3dx=41. However, this is multiplied by an additional factor of
n1:
L2=n→∞lim(n1⋅41)=0⋅41=0
The higher power in the denominator effectively causes the sum of cubes to vanish in the limit. Combining our results, we find:
L1−L2=51−0=51
This approach demonstrates that understanding the growth rates and the geometry of Riemann sums is far more efficient than algebraic expansion.