1.12 Solution to the Additional Problems
- First partial derivatives: ∂E2∂A=∫303∂∂A(6.1(x+5.0)e−0.045x−Ax−B)2dx=2∫303(6.1(x+5.0)e−0.045x−Ax−B)(−x)dx Equating to zero and dividing by 2 gives 0=−∫3036.1(x−2+5x)e−0.045xdx+∫303Ax2+Bxdx Successive integration by parts (for the first integral) and direct integration (for the second integral) yield the first equation: 0=8991.0A+445.5B−25984.9 ∂E2∂B=∫303∂∂B(6.1(x+5.0)e−0.045x−Ax−B)2dx=−2∫303(6.1(x+5.0)e−0.045x−Ax−B)dx
Equating to zero, dividing by 2 and solving yields the second equation: 0=445.5A+27.0B−1568.8
The solutions are A=0.061, B=57.1. The least squares integral using the approximation Y=0.061x+57.1 is 546.452.
- Let x=asinθ. The limits of integration are then changed as follows −a≤x≤a −a≤asinθ≤a −1≤sinθ≤1
There are many options for the range of θ. We first change the integrand to see which range is suitable. We know the integrand is non-negative since x2≤a2. Substitution gives
x=asinθ
dx=acosθdθ
√a2−x2dx=√a2−a2sin2θ⋅acosθdθ
The integrand is then non-negative when the positive square root is used and when cosθ is non-negative. Thus, we choose the limits of integration to be −π2, π2 since sin(−π2)=1,sin(π2=1) and cosθ≤0 if −π2≤θ≤π2.
The integral is then
∫π/2−π/2√a2−a2sin2θacosθdθ=a2∫π/2−π/2√1−sin2θcosθdθ
=a2∫π/2−π/2cos2θdθ=a2[θ2+sin2θ4]π/2−π/2=a2[π/4+(1/4)(0)−(−π/4)−(1/4)(0)]=πa2/2
Thus
A=2ba∫a−a√a2−x2dx=πab
When a=b=5.57, A=97.47.
When a=5, b=6.09, A=95.66.
From the right-hand diagram, we have cosR=B/x and thus x=B/cosR The minor axis is then the circle’s diameter, B. In the answer to part “a”, we replace 2a by B/cosR and 2b by B.
A=πab=π(B/2cosR)(B/2)=πB2/(4cosR)
Since the area of the circle is πB2/4,the dilution coefficient is
D=πB2/4πB2/4cosR=cosR
Thus D=0.6 means less dilution than D=0.3, and D=1.0 means no dilution at all. For Minnesota, the coefficients are
D=0.94 for R=20°
D=0.42 for R=65°