Analyzing the Setup
We start by translating our geometric reality into the language of calculus. The area under a curve y=f(x) from a lower limit a to an upper limit b is defined by the definite integral ∫abf(x)dx.
In our case, the lower limit is fixed at 1, and the upper limit is b. We can express this relationship as:
∫1bf(x)dx=(b−1)sin(3b+4)
This equation is our starting point. The function f(x) is currently 'trapped' inside the integral, and we must use inverse operations to set it free.
The Surgical Tool
The Leibniz Rule
To differentiate an integral with a variable limit, we use the Newton-Leibniz Rule. This tool allows us to peek inside the integral and isolate the integrand.
The rule states:
dbd∫g(b)h(b)f(x)dx=f(h(b))⋅h′(b)−f(g(b))⋅g′(b)
Here, our lower limit g(b)=1 is a constant, and our upper limit h(b)=b. Since the derivative of a constant is zero, the derivative of the left-hand side simplifies beautifully to just f(b).
The Execution
The Product Rule Dance
Now, we must differentiate the right-hand side, (b−1)sin(3b+4), with respect to b. This requires the Product Rule: dbd(u⋅v)=u⋅v′+v⋅u′.
Let u=(b−1) and v=sin(3b+4). The derivative of u is 1, while the derivative of v (using the Chain Rule) is 3cos(3b+4).
Combining these components, we obtain:
f(b)=(b−1)⋅3cos(3b+4)+sin(3b+4)⋅1
Simplifying this expression, we arrive at the identity of the function in terms of b:
f(b)=sin(3b+4)+3(b−1)cos(3b+4)
The Final Reveal
We have successfully extracted the function. Since b was merely a placeholder for the variable limit, we replace b with x to find the general form of our function:
f(x)=sin(3x+4)+3(x−1)cos(3x+4)
This result demonstrates the elegance of calculus. By applying the fundamental relationship between integration and differentiation, we have successfully solved the mystery of the trapped function.