Let R be the first quadrant region enclosed by the graph of y= 2e^-x and the line x=k.

a) Find the area of R in terms of k.

b) Find the volume of the solid generated when R is rotated about the x-axis in terms of k.

c) What is the volume in part (b) as k approaches infinity?

To find the area of the region R in terms of k:

Step 1: Set up the integral limits for the region R.

Since R is the first quadrant region enclosed by the graph of y = 2e^-x and the line x = k, we need to find the intersection point of the two curves.

Setting y = 2e^-x equal to the equation of the line x = k, we have:
2e^-x = k

Taking the natural logarithm of both sides gives:
-ln(2) - x = ln(k)

Simplifying, we find:
x = -ln(k) - ln(2)

So the integral limits for the region R are x = 0 (the y-axis) and x = -ln(k) - ln(2) (the intersection point).

Step 2: Set up the integral expression for the area of R.

The area of R can be calculated using the integral of the function y = 2e^-x from the lower limit to the upper limit:

Area = ∫[0, -ln(k) - ln(2)] 2e^-x dx

Step 3: Evaluate the integral.

Integrating 2e^-x gives:
Area = [2(-e^-x)] evaluated from 0 to -ln(k) - ln(2)
= 2(-e^-(-ln(k) - ln(2))) - 2(-e^0)
= 2(-e^(ln(k) + ln(2))) - 2(-1)
= 2(-e^(ln(k)) * e^(ln(2))) + 2
= 2(-k * 2) + 2
= -4k + 2

So the area of R in terms of k is -4k + 2.

To find the volume of the solid generated when R is rotated about the x-axis in terms of k:

Step 1: Set up the integral limits for the volume.

Since R is being rotated around the x-axis, the volume can be calculated using the disk method. The radius of the disk is given by the function, y = 2e^-x.

The integral limits for the volume are the same as for the area calculation, x = 0 and x = -ln(k) - ln(2).

Step 2: Set up the integral expression for the volume.

The volume V can be calculated using the integral of the function for the area of a circle (πr^2) from the lower limit to the upper limit:

V = ∫[0, -ln(k) - ln(2)] π(2e^-x)^2 dx
= ∫[0, -ln(k) - ln(2)] π(4e^-2x) dx
= π∫[0, -ln(k) - ln(2)] 4e^-2x dx

Step 3: Evaluate the integral.

Integrating 4e^-2x gives:
V = π[(-1/2)e^-2x] evaluated from 0 to -ln(k) - ln(2)
= π[(-1/2)e^-2(-ln(k) - ln(2))) - (-1/2)e^-2(0)]
= π[(-1/2)e^(2ln(k) + 2ln(2))] - π(-1/2)

Expanding the exponential term, we get:
V = π[(-1/2)(e^(ln(k)^2) * e^(ln(2)^2))] - π(-1/2)
= π[(-1/2)(k^2 * 2^2)] - π(-1/2)
= π[(-1/2)(4k^2)] - π(-1/2)
= -2πk^2 + π/2

So the volume of the solid generated when R is rotated about the x-axis in terms of k is -2πk^2 + π/2.

To find the volume as k approaches infinity:

As k approaches infinity, the term -2πk^2 dominates, so the volume approaches negative infinity.

Therefore, the volume as k approaches infinity is negative infinity.

To find the area and volume in terms of k, we first need to locate the points of intersection between the graph of y = 2e^-x and the line x = k.

To find the point of intersection, we set the equations equal to each other and solve for x:

2e^-x = k

Now, let's solve each part of the question step by step:

a) Finding the Area of R in terms of k:

To find the area of R, we need to calculate the integral of 2e^-x from x = 0 to x = k. This will give us the area enclosed by the graph of y = 2e^-x and the line x = k:

Area_R = ∫[0,k] 2e^-x dx

To evaluate this integral, we can use integration by substitution.

Let u = -x, du = -dx.

Now, when x = 0, u = 0, and when x = k, u = -k.

Substituting the values and shifting the limits of integration:

Area_R = ∫[-k,0] 2e^u (-du)
= -∫[0,-k] 2e^u du
= -2∫[0,-k] e^u du
= -2[e^u]_[0,-k]
= -2[e^-k - e^0]
= -2[e^-k - 1]
= 2(1 - e^-k)

Therefore, the area of R in terms of k is given by 2(1 - e^-k).

b) Finding the Volume of the Solid when R is Rotated about the x-axis in terms of k:

To find the volume of the solid, we need to calculate the integral of the cross-sectional area of R from x = 0 to x = k, as the graph is rotated around the x-axis:

Volume = ∫[0,k] π(2e^-x)^2 dx
= ∫[0,k] 4πe^(-2x) dx

To evaluate this integral, we can use integration by substitution.

Let u = -2x, du = -2dx.

Now, when x = 0, u = 0, and when x = k, u = -2k.

Substituting the values and shifting the limits of integration:

Volume = ∫[0,-2k] 4πe^u (-du/2)
= -2π∫[0,-2k] e^u du
= -2π[e^u]_[0,-2k]
= -2π[e^(-2k) - e^0]
= -2π[e^(-2k) - 1]

Therefore, the volume of the solid when R is rotated about the x-axis in terms of k is given by -2π[e^(-2k) - 1].

c) Finding the Volume as k approaches infinity:

As k approaches infinity, the exponential term e^(-2k) approaches zero because the exponent becomes infinitely negative. Therefore, the volume can be approximated as:

Volume ≈ -2π(-1) = 2π

Therefore, as k approaches infinity, the volume of the solid approaches 2π.

a) For the first quadrant region, x>0 to x = k, and the enclosed area is

Integral y dx =
Integral 2e^-x dx
x = 0 to k
= -2 e^-k + 2 e^0
= 2(1 - e^-k)

b) Make the integrand pi*y^2 dx and perform the resulting integration from 0 to k

c) This should be obvious after doing (b)