Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a problem; we are peeling back the layers of a mathematical onion to reveal a hidden symmetry. We are given two sequences, Sn and Tn, and a complex-looking summation that seems designed to intimidate.
But fear not, for beneath the surface lies a beautiful, structured dance of algebra.
Decoding the Sequences
First, let us look at Sn=1+q+q2+⋯+qn. This is a classic Geometric Progression where the first term a=1 and the common ratio is q. Since the powers of q range from 0 to n, there are exactly n+1 terms.
Using the sum formula for a G.P., we obtain:
Now, consider Tn=1+(2q+1)+(2q+1)2+⋯+(2q+1)n. This is also a G.P., but with a common ratio r=2q+1. Applying the same logic, we find:
The Sigma Transformation
The given series is 101C1+101C2S1+⋯+101C101S100. We can express this using Sigma notation as ∑r=1101101CrSr−1.
Notice how the subscript of S is always one less than the index of C. Substituting our formula for Sr−1, we get:
Since q−1 is independent of r, we pull it out of the summation:
q−11r=1∑101101Cr(qr−1)
The Binomial Dance
Now, we distribute the binomial coefficient to split the sum into two distinct parts:
q−11[r=1∑101101Crqr−r=1∑101101Cr]
The first part is almost the binomial expansion of (1+q)101. The only missing piece is the r=0 term, which is 101C0q0=1. Thus, the first sum is (1+q)101−1.
The second part is the sum of binomial coefficients, which is 2101−1 (again, subtracting the r=0 term). Combining these, our LHS becomes:
q−1(1+q)101−1−(2101−1)=q−1(1+q)101−2101
The Grand Cancellation
Finally, we look at the RHS, αT100. Substituting n=100 into our Tn formula, we get:
T100=2q+1−1(2q+1)101−1=2101(q+1)101−2101⋅q−12=2100(q−1)(q+1)101−2101
Equating the LHS and RHS, we have:
q−1(1+q)101−2101=α2100(q−1)(q+1)101−2101
The massive term involving q cancels out perfectly, leaving 1=2100α. Therefore, the final result is: