To determine the correct statements, we first find the explicit form of the function f(x).
Step 1: Formulating and Solving the Differential Equation
The given integral equation is:
f(x)=1−2x+∫0xex−tf(t)dtfor all x∈[0,∞)
We can rewrite the integral by factoring out ex:
f(x)=1−2x+ex∫0xe−tf(t)dt
Multiplying both sides by e−x:
e−xf(x)=(1−2x)e−x+∫0xe−tf(t)dt
Differentiating both sides with respect to x using the product rule and Leibniz Rule:
e−xf′(x)−e−xf(x)=−2e−x−(1−2x)e−x+e−xf(x)
Since e−x=0 for all real x, dividing the entire equation by e−x yields:
f′(x)−f(x)=−3+2x+f(x)f′(x)−2f(x)=2x−3
This is a first-order linear differential equation of the form dxdy+P(x)y=Q(x) with:
Integrating Factor (I.F.)=e∫−2dx=e−2x
Multiplying both sides by the integrating factor:
dxd[f(x)e−2x]=(2x−3)e−2x
Integrating both sides with respect to x:
f(x)e−2x=∫(2x−3)e−2xdxf(x)e−2x=(2x−3)(−2e−2x)−∫2(−2e−2x)dxf(x)e−2x=−21(2x−3)e−2x−21e−2x+Cf(x)e−2x=(1−x)e−2x+C
Multiplying through by e2x:
f(x)=1−x+Ce2x
Step 2: Determining the Constant C
From the original integral equation, substituting x=0:
f(0)=1−2(0)+∫00e0−tf(t)dt=1
Using our solution for f(x):
f(0)=1−0+Ce0=1+C
Setting this equal to 1:
1+C=1⟹C=0
Thus, the continuous function is:
f(x)=1−x
Step 3: Checking the Options
Option (A):f(1)=1−1=0=2
Hence, the curve does not pass through (1,2). (Option A is FALSE)
Option (B):f(2)=1−2=−1
Hence, the curve passes through the point (2,−1). (Option B is TRUE)
Options (C) and (D):
We find the area of the region bounded by f(x)≤y≤1−x2 for x∈[0,1].
Since for all x∈[0,1], 1−x≤1−x2, the enclosed area A is given by:
A=∫01(1−x2−(1−x))dxA=∫011−x2dx−∫01(1−x)dx
∫011−x2dx represents the area of a quarter of a circle of radius 1:
∫011−x2dx=4π(1)2=4π