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对145页最下面那个极限应用洛必达法则,就得到了红线的式子。
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f(x)
= ; x≠0
=a ; x=0
(1)
lim(x->0) f(x)
=lim(x->0) [g(x) -cosx]/x (0/0 分子分母分别求导)
=lim(x->0) [g'(x) -sinx]
=g'(0)
=> a= g'(0)
(2)
f'(x)
=lim(h->0) [f(x+h) - f(x) ]/h
=lim(h->0) { [g(x+h) -cos(x+h)]/(x+h) - [g(x) -cosx]/x } /h
=lim(h->0) {x [g(x+h) -cos(x+h)] -(x+h) [g(x) -cosx] } /[x(x+h)h]
(0/0 分子分母分别求导)
=lim(h->0) {x [g'(x+h) +sin(x+h)] - [g(x) -cosx] } /[x(x+2h)]
={x[g'(x) +sinx] - [g(x) -cosx] } /x^2
= [ xg'(x) +xsinx -g(x) +cosx] /x^2
= ; x≠0
=a ; x=0
(1)
lim(x->0) f(x)
=lim(x->0) [g(x) -cosx]/x (0/0 分子分母分别求导)
=lim(x->0) [g'(x) -sinx]
=g'(0)
=> a= g'(0)
(2)
f'(x)
=lim(h->0) [f(x+h) - f(x) ]/h
=lim(h->0) { [g(x+h) -cos(x+h)]/(x+h) - [g(x) -cosx]/x } /h
=lim(h->0) {x [g(x+h) -cos(x+h)] -(x+h) [g(x) -cosx] } /[x(x+h)h]
(0/0 分子分母分别求导)
=lim(h->0) {x [g'(x+h) +sin(x+h)] - [g(x) -cosx] } /[x(x+2h)]
={x[g'(x) +sinx] - [g(x) -cosx] } /x^2
= [ xg'(x) +xsinx -g(x) +cosx] /x^2
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