Analyzing the Setup
The given integral is defined as:
g(x)=∫xπ/2[f′(t)csct−cottcsctf(t)]dt
At first glance, this expression appears complex. However, we must look for underlying relationships between the functions f(t) and the trigonometric terms.
The Detective Work
Recall the product rule for differentiation:
dtd[u(t)v(t)]=u′(t)v(t)+u(t)v′(t)
If we set u(t)=f(t) and v(t)=csct, we note that the derivative of v(t) is v′(t)=−csctcott.
Substituting these into the product rule, we get:
dtd[f(t)csct]=f′(t)csct−f(t)csctcott
This matches the integrand perfectly. The entire expression is simply the derivative of the product f(t)csct.
The Fundamental Theorem
By the Fundamental Theorem of Calculus, the integral of a derivative is the original function. We evaluate the expression at the given boundaries:
g(x)=f(π/2)csc(π/2)−f(x)cscx
Since csc(π/2)=1, the expression simplifies to:
The Final Limit
We now evaluate the limit as x→0:
x→0limg(x)=x→0lim[f(π/2)−sinxf(x)]
The term f(π/2) is a constant. The term sinxf(x) presents an indeterminate form of 00 because f(0)=0 and sin0=0.
Applying L'Hopital's Rule, we differentiate the numerator and denominator:
x→0limcosxf′(x)=cos0f′(0)=11=1
Given the condition f(π/2)=3, we perform the final subtraction:
The final result is 2.