Now define the linear maps L = f′(x0) and M = g′(y0) to be the derivatives of f and g, respectively, at x0 and y0. Thus we have
and
via the combination of the differentiability of f and g and our assumption that x0, f(x0) = y0, and g(y0) = z0 are all at the origin of their respective spaces. These two equations then yield the following sequence of equations for sufficiently small x ∈ Rm
Hence if we can show that is bounded as |x|→ 0, then the previous inequality implies that can be arbitrarily bounded as |x|→ 0. Such a property on proves our theorem since
as we assumed x0 is the origin.
So to, finally, prove the boundedness of |f(x)|∕|x| we see that
but |L(x)|∕|x| < |L| and → 0 as |x|→ 0. Hence is bounded as |x|→ 0 as desired.
and then define E : U → R by
Due to the definition of gh we can apply the mean value theorem (MVT) to E twice, but in two different ways:
for some 0 ≤ t1 ≤ 1. We next expand gh in the result to obtain
and finally apply the MVT once more now to f to get
| (2.1) |
for some 0 ≤ s1 ≤ 1.
and then apply the MVT first to the resulting expansion of the first component and then a second time to the resulting expansion of the second component to get
| (2.2) |
for some 0 ≤ t2 ≤ 1.
Therefore equations 2.1 and 2.2 yield
| (2.3) |
Now in light of the definition of E, we see that E is also continuous in both h and k so that letting h → 0 followed by letting k → 0 will have the same value as letting k → 0 followed by letting h → 0. Thus we can let h → 0 and k → 0, safely in either order, in equation 2.3 to obtain
as desired.
| (3.4) |
Since this is true for any t ∈ R, setting t = 1 yields xfx(x,y) + yfy(x,y) = nf(x,y), as desired.
which becomes
upon expanding and combining like terms. Thus by, once more, evaluating this formula at t = 1 we obtain the desired formula.
so we need to confirm the formulas from the previous part of the problem. For xfx + yfy we get
Now we need to confirm the second formula. To start, we have
so that
as desired.
Prove that f is differentiable for all x, including x = 0, but the derivative f′(x) is not continuous at x = 0.