Given F(x)=∫0xf(t)dt, so F′(x)=f(x) and F′′(x)=f′(x).
The integral is ∫0π[f′(x)+F(x)]cosxdx=∫0πf′(x)cosxdx+∫0πF(x)cosxdx.
Evaluate ∫0πf′(x)cosxdx by parts: u=cosx, dv=f′(x)dx, so du=−sinxdx, v=f(x).
Then ∫0πf′(x)cosxdx=[cosxf(x)]0π+∫0πf(x)sinxdx=(cosπf(π)−cos0f(0))+∫0πf(x)sinxdx=(−1)(−6)−(1)f(0)+∫0πf(x)sinxdx=6−f(0)+∫0πf(x)sinxdx.
Evaluate ∫0πF(x)cosxdx by parts: u=F(x), dv=cosxdx, so du=f(x)dx, v=sinx.
Then ∫0πF(x)cosxdx=[F(x)sinx]0π−∫0πf(x)sinxdx=(F(π)sinπ−F(0)sin0)−∫0πf(x)sinxdx=0−0−∫0πf(x)sinxdx=−∫0πf(x)sinxdx.
Adding: ∫0π[f′(x)+F(x)]cosxdx=[6−f(0)+∫0πf(x)sinxdx]+[−∫0πf(x)sinxdx]=6−f(0).
Given equals 2, so 6−f(0)=2⇒f(0)=4.