Key Concepts and Formulas
- Summation of Powers:
- ∑r=1kr=2k(k+1)
- ∑r=1kr2=6k(k+1)(2k+1)
- Factorial Properties:
- n!=n⋅(n−1)!
- n!=n⋅(n−1)⋅(n−2)!
- Taylor Series Expansion of ex: The series for ex centered at 0 is ∑k=0∞k!xk. For x=1, this gives e=∑k=0∞k!1.
Step-by-Step Solution
Step 1: Express Sn in Summation Notation and Derive its Closed Form.
The given sum is Sn=1⋅(n−1)+2⋅(n−2)+3⋅(n−3)+⋯+(n−1)⋅1.
We can observe that the general term is of the form r⋅(n−r), where r ranges from 1 to n−1.
So, Sn=∑r=1n−1r(n−r).
Expanding the term inside the summation, we get r(n−r)=nr−r2.
Thus, Sn=∑r=1n−1(nr−r2).
Using the linearity of summation, we can split this into two sums:
Sn=n∑r=1n−1r−∑r=1n−1r2.
Now, we apply the standard summation formulas for the sum of the first k integers and the sum of the first k squares, with k=n−1:
Sn=n(2(n−1)((n−1)+1))−(6(n−1)((n−1)+1)(2(n−1)+1))
Sn=n(2(n−1)n)−(6(n−1)n(2n−1))
Sn=2n2(n−1)−6n(n−1)(2n−1).
To simplify, we find a common denominator (6) and factor out common terms:
Sn=63n2(n−1)−6n(n−1)(2n−1)
Sn=6n(n−1)[3n−(2n−1)]
Sn=6n(n−1)[3n−2n+1]
Sn=6n(n−1)(n+1).
Why this step? Deriving a closed-form expression for Sn simplifies the subsequent calculations and allows us to work with a more manageable algebraic form.
Step 2: Simplify the General Term of the Infinite Sum.
The general term of the infinite sum is (n!2Sn−(n−2)!1).
Substitute the derived expression for Sn:
2Sn=2⋅6n(n−1)(n+1)=3n(n−1)(n+1).
Now, substitute this into the general term:
3n!n(n−1)(n+1)−(n−2)!1.
We use the factorial property n!=n(n−1)(n−2)! to simplify the first term:
3⋅n(n−1)(n−2)!n(n−1)(n+1)−(n−2)!1.
Cancel the common factors n(n−1) in the first term:
3(n−2)!n+1−(n−2)!1.
To combine these terms, we ensure a common denominator, which is 3(n−2)!:
3(n−2)!n+1−3(n−2)!3.
Combine the numerators:
3(n−2)!(n+1)−3=3(n−2)!n−2.
Now, use the factorial property (n−2)!=(n−2)(n−3)! (since n≥4, n−2≥2, so this is valid):
3(n−2)(n−3)!n−2.
Cancel the common factor (n−2):
3(n−3)!1.
Why this step? Simplifying the general term of the infinite sum into a compact form involving factorials is crucial for recognizing its connection to known series expansions.
Step 3: Evaluate the Infinite Sum.
The infinite sum is ∑n=4∞(n!2Sn−(n−2)!1).
Using the simplified general term from Step 2, the sum becomes:
∑n=4∞3(n−3)!1.
Factor out the constant 31:
31∑n=4∞(n−3)!1.
To relate this to the Taylor series for e, we change the index of summation. Let k=n−3.
When n=4, k=4−3=1.
As n→∞, k→∞.
The sum transforms to:
31∑k=1∞k!1.
The Taylor series for e is e=∑k=0∞k!1=0!1+1!1+2!1+….
Our sum is ∑k=1∞k!1=1!1+2!1+3!1+….
This is the series for e minus its k=0 term:
∑k=1∞k!1=(∑k=0∞k!1)−0!1.
Since 0!1=1, we have:
∑k=1∞k!1=e−1.
Substituting this back into our expression:
31(e−1)=3e−1.
Why this step? By manipulating the summation index and recognizing the form of the Taylor series for e, we can evaluate the infinite sum.
Common Mistakes & Tips
- Index Errors: Be extremely careful when changing summation indices. Ensure the starting, ending, and incremental steps of the new index correctly map to the original index.
- Taylor Series for e: Remember that e=∑k=0∞k!1=1+∑k=1∞k!1. A common mistake is to equate ∑k=1∞k!1 directly with e without subtracting the k=0 term.
- Algebraic Simplification: Errors in simplifying Sn or the general term of the infinite sum will propagate. Double-check all algebraic manipulations, especially with factorials.
Summary
The problem required finding the value of an infinite sum. We first derived a closed-form expression for Sn using summation formulas. Then, we simplified the general term of the infinite sum by substituting the expression for Sn and utilizing factorial properties. Finally, by recognizing the resulting series as a part of the Taylor expansion of e, we evaluated the infinite sum.
The final answer is 3e−1 which corresponds to option (A).