By way of preparation, we have
∂x∂T(x,y)=2xey∂y∂T(x,y)=ey(x2+y2+2y) (a) (i)
For this problem the objective function is T(x,y)=ey(x2+y2)
and the constraint function is g(x,y)=x2+y2−100.
According to the method of Lagrange multipliers, Theorem 16.3.2
in the text, we need to find all solutions to
TxTyg(x,y)=λgx=λgy=1002xeyey(x2+y2+2y)x2+y2=λ(2x)=λ(2y)=100(E1)(E2)(E3) If gx=0 and gy=0, then (E1) λ=ey and (E2) λ=2yey(x2+y2+2y).
ey2y0=2yey(x2+y2+2y)=x2+y2+2y=x2+y2 but this conflicts with (E3). So gx=0 and gy=0 doesn't lead to any solutions.
If gx=0, then x=0 and (E1) is true; then we can choose the appropriate λ to make (E2) true. From (E3), y=±10. So (0,±10) gives a solution.
If gy=0, then y=0. By (E2), x=0, which conflicts with (E3).
So the only possible locations of the maximum and minimum of the function
T are (0,10) and (0,−10). To complete this part of the problem, we only have to
compute T at those points.
| point | (0,10) | (0,−10) |
| value of T | 100e10 | 100e−10 |
| max | min |
Hence the maximum value of T(x,y)=ey(x2+y2) on x2+y2=100
is 100e10 at (0,10) and the minimum value is 100e−10 at (0,−10).
We remark that, on x2+y2=100, the objective function
T(x,y)=ey(x2+y2)=100ey. So of course the maximum value of
T is achieved when y is a maximum, i.e. when y=10,
and the minimum value of
T is achieved when y is a minimum, i.e. when y=−10.
(b) (i) By definition, the point (x,y) is a critical point of T(x,y) if and only if the first order partial derivatives at that point are both zero, or at least one does not exist. The first partial derivatives
TxTy=2xey=ey(x2+y2+2y) are well defined everywhere and so the critical points are exactly the point where
Tx=2xeyTy=ey(x2+y2+2y)=0=0(E1)(E2) (b) (ii)
Equation (E1) forces x=0. When x=0, equation (E2) reduces to
ey(y2+2y)=0⟺y(y+2)=0⟺y=0 or y=−2 So there are two critical points, namely (0,0) and (0,−2).
(c)
Note that T(x,y)=ey(x2+y2)≥0 on all of R2.
As T(x,y)=0 only at (0,0), it is obvious that (0,0) is the coolest point.
In case you didn't notice that, here is a more conventional solution.
The coolest point on the solid disc x2+y2≤100
must either be on the boundary, x2+y2=100, of the disc
or be in the interior, x2+y2<100, of the disc.
In part (a) (ii) we found that the coolest point on the boundary
is (0,−10), where T=100e−10.
If the coolest point is in the interior, it must be a critical point and so must be
either (0,0), where T=0, or (0,−2), where T=4e−2.
So the coolest point is (0,0).