Proof about sum of indices of singular points In Lee's Topological Manifolds, problem 8-10 discusses vector fields in the plane, and defines them as continuous maps $v:\mathbb{R}^2\rightarrow\mathbb{R}^2$. An isolated singular point is a point $p$ where $v(p)=0$, but there is an open set $p\in U$ so that $v^{-1}(0)\cap U=\{p\}$.
The first two parts of the problem show we can define the index of $p$ as follows: find a small circle $C\in U$ around $p$, and consider the map $v: C\rightarrow\mathbb{R}^2-\{0\}$. The index of $p$ is then the winding number of this map.
The third part of the problem is as follows (and where my question lies): Suppose $p_1,\ldots,p_n$ are all the isolated singular points of $v$, all contained in the open unit disk of $\mathbb{R}^2$.  Let $S^1$ be the boundary of the unit disk.  Show the sum of the indices of the $p_i$ is equal to the winding number of $v(S^1)$.
I have this idea that I could "shrink-wrap" $S^1$ down to loops around the $p_i$, and then show the parts connecting the loops cancel each other out, winding number-wise.  But this is pretty hand-wavy.  Is there a more formal way to prove this? I'm happy even to get a hint in the right direction.
(Sorry for all the setup, but there are lots of ways to define winding number, and I didn't want to use something not discussed in the book)
 A: As Lee defines, if $v$ has an isolated zero at $p$, and if $C$ is a circle of radius $\varepsilon$ around $p$ in $\Bbb R^2$, then $v|_C : C \to \Bbb R^2 \setminus 0$ is a loop around the origin, and the index of $v$ at $p$ is precisely the winding number of $v|_C$ given by the formula (where the division is defined after identifying $\Bbb R^2$ with $\Bbb C$)
$$\iota_p(v) = \frac{1}{2\pi i} \int_C \frac{v'(s)}{v(s)} ds$$ 
It's worth noting that this formula works because, roughly, "$v'(s)/v(s) ds = d\log v(s)$" where $\log$ is a multivalued function defined on $\Bbb C \setminus 0$ which changes it's argument by $\pm 2\pi i$ if one goes a circle counterclockwise or clockwise around the origin. Therefore $\iota_p(v)$ is a sum over $\pm 1$'s corresponding to counterclockwise or clockwise rotations of $v|_C$ around the origin, which sums to the total number of counterclockwise rotations of $v|_C$ around $0$. Notice also that by the change of variables formula we could write $$\frac{1}{2\pi i} \int_C \frac{v'(s)}{v(s)} ds = \frac{1}{2\pi i}\int_{\gamma} \frac{dz}{z}$$ where $\gamma$ is the loop $v(C)$ parameterized by the map $v|_C$.
Suppose now that $p_1, \cdots, p_n$ are isolated zeroes of $v$ contained in the disk $D^2$. Let $C_1, \cdots, C_n$ be circles of radius $\varepsilon$ around these zeroes contained in $D^2$, which we can manage to do by choosing $\varepsilon > 0$ appropriately. Further, let's go by your suggestion in the question and delete arcs $\mathcal{A}_i$ and $\mathcal{A}'_i$ on $\partial D^2$ and $C_i$ respectively and add in tubes $T_i$ connecting $\partial D^2$ and $C_i$ by inserting it between the deleted arcs, roughly like the following picture (I haven't deleted the arcs while drawing, oops): 

Then we have a loop $\ell$ given by the union of all these little pieces (i.e., traversing $\partial D^2 - \bigcup_i \mathcal{A}_i$, the tubes $T_i$ and then the circles $C_i - \mathcal{A}_i'$, in counterclockwise order) which does not contain any zero of $v$ inside it by construction. Therefore the winding number of $v$ along $\ell$ is $$\frac{1}{2\pi i} \int_{\ell} \frac{v'(s)}{v(s)} ds = \frac{1}{2\pi i} \int_{v(\ell)} \frac{dz}{z} = 0$$ by Cauchy's theorem as $1/z$ is holomorphic inside $v(\ell)$, which is a loop that does not contain the origin. We can expand the integral out as follows (here the integral over the circles $C_i$ gets a sign because if $\ell$ is traversed counterclockwise then $C_i$ is oriented clockwise)
$$\frac{1}{2\pi i} \left ( \int_{\partial D^2 - \bigcup_i \mathcal{A}_i} \frac{v'(s)}{v(s)} ds + \sum_{i} \int_{T_i} \frac{v'(s)}{v(s)} ds + \sum_{i} -\int_{C_i - \mathcal{A}_i'} \frac{v'(s)}{v(s)} ds \right ) = 0$$
If we write $T_i = I^1_i \cup I^2_i$ where $I^1_i$ and $I_i^2$ are the parallel lines that constitute the tube (oppositely oriented), then as we decrease the width of the tube i.e., let $\delta \to 0$, we get
$$\int_{T_i} \frac{v'(s)}{v(s)} ds = \int_{I^1_i} \frac{v'(s)}{v(s)} ds - \int_{I^2_i} \frac{v'(s)}{v(s)} ds \to 0$$ 
Therefore we can take the middle term to vanish and as letting $\delta \to 0$ also shrinks the removed arcs $\mathcal{A}_i, \mathcal{A}_i'$, we can forget about them too. Therefore rearranging the rest gives $$\frac{1}{2\pi i} \int_{\partial D^2} \frac{v'(s)}{v(s)} ds = \frac1{2\pi i} \left (\int_{C_1} + \cdots + \int_{C_n} \right ) \frac{v'(s)}{v(s)} ds$$ which proves that the winding number of $v$ along $\partial D^2$ is $\iota_{p_1}(v) + \cdots + \iota_{p_n}(v)$, as required.
A: Choose real numbers $0<r_1<\cdots <r_k=1$ with the following properties:


*

*$V(z)\neq 0$ if $|z|=r_j$;

*The singular points of $V$ that lie in the annulus $A_j:=\{z\in\mathbb C|r_{j}< z<r_{j+1}\}$  (we define $A_0$ to be the open ball of radius $r_1$ centered at the origin) all have the same modulus. 


Define $f_j:I\to\mathbb{B}^2$ to be the loop $f_j(t)=r_je^{2\pi it}$. It is not hard to convince ourselves that the difference $N(V,f_{j+1})-N(V,f_j)$ of winding numbers of $V$ equals the sum of indices of $V$ at the singular points in $A_j$. By telescoping series, we obtain our results.
