Analyzing the Setup
The series is given by ∑n=1∞(2n+1)!n2+6n+10. At first glance, the quadratic numerator over a factorial denominator suggests an exponential series structure.
The presence of (2n+1)! is a significant hint. We recall the standard Taylor series for ex and e−x:
e=k=0∑∞k!1,e−1=k=0∑∞k!(−1)k
The Factorial Trap
To simplify the expression, we perform a substitution. Let r=2n+1. As n ranges from 1 to ∞, r takes the values 3,5,7,… (all odd integers starting from 3).
From r=2n+1, we have n=2r−1. Substituting this into the numerator n2+6n+10:
(2r−1)2+6(2r−1)+10=4r2−2r+1+3(r−1)+10
Simplifying the expression with a common denominator of 4:
4r2−2r+1+12r−12+40=4r2+10r+29
The Art of Decomposition
We now express the general term Tr as:
To facilitate summation, we decompose the numerator r2+10r+29 into terms that allow cancellation with r!:
Substituting this back into Tr:
Tr=41(r!r(r−1)+r!11r+r!29)=41((r−2)!1+(r−1)!11+r!29)
The Summation Dance
We sum over odd r∈{3,5,7,…}. We utilize the known series for odd and even positions:
Sum of odd factorials: ∑k oddk!1=2e−e−1
Sum of even factorials: ∑k evenk!1=2e+e−1
1. For ∑(r−2)!1 where r=3,5,…: This is 1!1+3!1+⋯=2e−e−1.
2. For ∑(r−1)!1 where r=3,5,…: This is 2!1+4!1+⋯=(2e+e−1−0!1)=2e+e−1−2.
3. For ∑r!1 where r=3,5,…: This is 3!1+5!1+⋯=(2e−e−1−1!1)=2e−e−1−2.
Final Calculation
Combining these results into the sum S:
S=41[2e−e−1+11(2e+e−1−2)+29(2e−e−1−2)]
Factoring out 21:
S=81[(1+11+29)e+(−1+11−29)e−1−22−58]
The final result is: