This is a problem from Semi-Riemannian Geometry by Barrett O'Neill.
For a smooth manifold $M$, we denote by $\mathcal{F}(M)$ the set of all smooth functions $f:M\rightarrow \mathbb{R}$, and by $T(M)$ the tangent bundle of $M$. I'm asked to prove the following:
Let $f \in \mathcal{F}(M)$. Then, the differential $df:T(M)\rightarrow\mathbb{R}$ and the differential map $df:T(M)\rightarrow T(\mathbb{R^1})$ differ only by a canonical isomorphism.
I find this a bit confusing since, initially I thought the differential and the differential map were obviously the same thing but I guess this is the whole point of the problem. Also I'm not familiar with the definition of a canonical isomorphism, the book gives two examples which I don't find to be all that illustrative. Any help/tips are appreciated.
Given a smooth map $f : M \to N$, its differential map $df$ is a map from the tangent bundle $T(M)$ to the tangent bundle $T(N)$. It is given fiberwise by the differential maps $df_p : T_p(M) \to T_{f(p)}(N)$ at the points $p \in M$. In the sequel let us write $T_p(f)$ instead of $df_p$ for distinction.
The differential of $f \in \mathfrak{F}(M)$ is the one-form $df$ which assigns to each point $p \in M$ the element $df_p$ of the cotangent space $T_p(M)^*$ given by $df_p(v) = v(f)$ for all $v \in T_p(M)$. Hence $df_p$ is a linear map $T_p(M) \to \mathbb{R}$ , and we may regard the collection of these $df_p$ as a map $df : T(M) = \bigcup_{p\in M} T_p(M) \to \mathbb{R}$. In my opinion this is not explained very well in your textbook.
Exercise 13 therefore does not really make sense. In fact each $f \in \mathfrak{F}(M)$ is nothing else than a smooth map $f : M \to \mathbb{R}$ so that it has a differential map $T(f) : T(M) \to T(\mathbb{R})$. However, $\mathbb{R}$ cannot be identified with the tangent bundle $T(\mathbb{R})$, hence the maps in question do not differ only by a canonical isomorphism.
What is meant is this: For each $p \in M$ we can compare the maps $T_p(f) : T_p(M) \to T_{f(p)}(\mathbb{R})$ and $df_p : T_p(M) \to \mathbb{R}$. But for each $y \in \mathbb{R}$ there is a canonical isomorphism $h_y :\mathbb{R} \to T_y(\mathbb{R})$ (see the section "Vector Spaces as Manifolds"). Then we get $h_{f(p)} df_p = T_p(f)$. This is now really a nice exercise in putting together all definitions in your textbook.