The written portion of your first assignment is now available (below), which covers some of the fundamental tools we’ll be using in our class. Initially this assignment may look a bit intimidating but keep in mind a few things:

- The homework is not as long as it might seem: all the text in the big gray blocks contains supplementary, formal definitions that you do not need to know in order to complete the assignments.
- Moreover, note that you are required to complete
**only three problems from each section**. - If the \(\wedge\) and \(\star\) symbols look alien to you, don’t sweat: this is
*not*something you should know already! We’ll be talking about these objects in our lectures next week. Until then, you can (and should) get a jump on the lectures by reading the first few sections of Chapter 3 in our course notes.

Finally, don’t be shy about asking us questions here in the comments, via email, or during office hours. *We want to help you succeed* on this first assignment, so that you can enjoy all the adventures yet to come…

Here is a zip file with the $\LaTeX$ source.

Exercise 10 appears to contain typos- The prompt defines only vector fields $U,V$ but the questions refer to vector fields $U,V,W$.

Good catch! Exercise 10 has been corrected.

Could you please also release the Latex file of Assignments?

Thanks!

I just released the source files.

where is the source file released ?

The source files had gotten out of sync with the official PDF, so they had been taken down. The up-to-date zip file has been added back to the above post.

Quick questions about a few typos (maybe?):

In exercise 17, is the orientation of the edge $(A,B)$ correct? It seems to be inconsistent with the orientation of the face $(A,D,B)$, but I may have misunderstood how orientations of edges and faces are supposed to behave with respect to one another.

In exercise 18, part (c), should the second wedge product be $\wedge_{1,0}$ (and not $\wedge_{2,0}$)?

In exercise 19, should $g$ be a 0-form, or should $\hat{g}$ be a discrete 1-form perhaps? Otherwise I’m not too sure how to evaluate a 1-form at vertices.

Thank you!

Those are good questions.

17) The orientations of the faces and edges do not need to be consistent (it’s a coincidence that only one of the edges is flipped the other way).

18) Great catch! It should be $\wedge_{1, 0}$ as written. There should be an extra $d$.

19) Good eye! 🙂 I meant for $g$ to be a $0$-form.

I’ve uploaded an updated PDF.

In class today you mentioned a possible extension on this assignment, so when exactly is this assignment going to be due now?

It’s already been updated on the calendar and the written assignment PDF; in the end we only added an extra day, because otherwise it becomes too hard to get the *next* assignment done in a reasonable amount of time. But we’ll continue to adjust as needed.

Just wanna squeeze out an extra credit from your preplanted landmines. There is no big deal.

In V4-1, Exercise 14 Exactness, if $f(x)=x^3$ then it SHOULD have the property that $\frac{d^2}{d x^2} f = 6x$ instead of the written one with $2x$.

That’s correct. I’ve fixed the exercise.

I am lost here. I’ll write my current thoughts and please tell me where I am getting something wrong here.

1) A cross product in R3 is a vector normal to the inputs with length equals area.

2) A cross product in R2 is just the number, that we interpret as form (or as an oriented area)

3a) The wedge product between vectors is the cross product.

or

3b) The wedge product is similar to cross product but substitutes the internal multiplication of the components by wedge products

4) In both 3a or 3b, there is a precise way to calculate a wedge between two vectors. However, how do you determine the wedge product between a form and a vector. I do not get if is there any coherent method for calculation or we should interpret the results case by case?

Thanks for writing down your thought process.

1) Yes, this is accurate.

2) You can think of a 2D cross product as a “number” or (0-vector), but this is not quite the same thing as a form.

3) Between (3a) and (3b), (3b) is the more accurate of the two. Note that the wedge product of two 1-vectors is a 2-vector, but the cross product in $\mathbb R^3$ takes two 1-vectors and makes another 1-vector. Therefore they are not the same operation but are highly related. Can you write down such a relationship using exterior calculus? (Hint: what relates 2-vectors and 1-vectors in $\mathbb R^3$?)

4) A form and vector are different types of objects, so you cannot take the wedge product of a form and a vector. Instead, you can

applya form to a vector in order to get a number. How to do this will be discussed in the next lecture (or you can read the posted slides).a) Please, can you show me a a concrete example comparing a wedge product and cross product?

b) Besides, the notion of a k-form is confusing for me. The text refers to the 1-form as different things:

1) the unit orthogonal 1-form $\alpha$ (kind of a vector)

2) a function $\alpha()$ 1-form that projects a given vector onto (1)

3) the result $\alpha(u)$ of the projection made by the function (2) onto (1).

a) Suppose we have two vectors in \(R^3\): \(u := e_1 + e_2 – 2e_3\) and \(v := 3e_1 + e_3\). Then \(u \times v = e_1 – 7e_2 – 3e_3\) and \(u \wedge v = (e_1+e_2-2e_3) \wedge (3e_1 + e_3)\) which when expanded becomes \(e_1 \wedge e_3 + 3 e_2 \wedge e_1 + e_2 \wedge e_3 – 6e_3 \wedge e_1\). Simplifying this expression we get the final answer \(u \wedge v = e_2 \wedge e_3 – 7e_3 \wedge e_1 – 3e_1 \wedge e_2\).

b) A 1-form is a linear map from a vector to a scalar. So, in your three examples, \(\alpha\) by itself is the 1-form; \(\alpha(u)\) is the result of applying the 1-form to a vector (producing a scalar). (I’m not sure what you mean by (1).)

Hope that helps! 🙂

Thanks Keenan, your answer was really helpful.

$a_1$) Now I understand the operation. However, I still have few questions here:

is $u \wedge v$ should happen for a certain basis, right? In this case, should the operation you computed be represented $e_1 \wedge e_2 \wedge e_3 (u, v)$

$a_2$) Just to confirm. While we understand the result of the cross product in $R^3$ as a normal vector, the result of $u \wedge v$ in $R^3$ should add the components to represent the area of the plane, right?

$a_3$) In my point (1) I was referring to “we represent this plane via a pair of unit orthogonal 1-forms $\alpha$ and $\beta$”. Notice that they are treated as unit vectors representing the base of the space for the projection – not as the “projection” map (point 2: the right definition) or as the result of the mapping (my point 3).

$a_4$) Following your example, the anti-symmetry property holds for the wedge product of the components $e_i$ or for the wedge product of vectors in $R^3$?

Well, that is all. Thanks again.

Hi Plav,

(a) I’m not sure what you mean about a basis. You do not *need* a basis in order to talk about wedge products. However, to do concrete calculations it is often convenient to write things in a basis. To make an analogy, you can understand what I mean if I say “add the vectors u and v”, even if I don’t explicitly expand u and v in a basis, i.e., I don’t need to write \(u = u_1 e_1 + u_2 e_2\) and \(v = v_1 e_1 + v_2 e_2\) in order for the expression “u+v” to make sense. Likewise, I don’t need to write u and v in components in order for the expression “u ^ v” to make sense. Geometrically, “u ^ v” means, “please give me a little patch of in space whose area is equal to the area of the parallelogram spanned by u and v, and which ‘points’ in the same direction as this parallelogram” (at least intuitively).

Also, you asked, “don’t you need to write it as \(e_1 \wedge e_2 \wedge e_3 (u,v,w)\). Here it’s important to understand the difference between exterior algebra (which we discussed in the previous lecture), and exterior calculus (which we will discuss in the next lecture). In exterior algebra, you *only* have wedge products, like “u ^ v”. You do not apply this wedge product to vectors. In exterior calculus, on the other hand, you can apply a wedge product to vectors, e.g., “\(\alpha \wedge \beta(u,v)\)”. In the former case, the wedge just represents a “little volume.” In the latter case, the wedge represents a “little volume *measurement*”.

If this is all a bit confusing, I wouldn’t worry—it takes a while for it to ‘sink in,’ and we haven’t even covered most of it in class! :-). But you’re asking the right kinds of questions.

(a2) Yes, the cross product \(u \times v\) and the wedge product \(u \wedge v\) are indeed different types of quantities. (I think this is a homework exercise, so I do not want to completely give away the solution! :-)). But also please be careful: you say that we should “add” the components of \(u\) and \(v\) to get the wedge product \(u \wedge v\). This is not quite true: we are not “adding”, but rather performing a completely different operation called the “wedge product.” For instance, if \(u\) and \(v\) are vectors in \(\mathbb{R}^2\) expressed as \(u := a e_1 + b e_2\) and \(v := c e_1 + d e_2\), then their wedge product is \(u \wedge v = (a e_1 + b e_2) \wedge (c e_1 + d e_2)\) and distributing the wedge over the product we get \((a e_1 + b e_2) \wedge (c e_1) + (a e_1 + b e_2) \wedge (d e_2) = ac \underbrace{e_1 \wedge e_1}_{=0} + bc \underbrace{e_2 \wedge e_1}_{=-e_1 \wedge e_2} + ad e_1 \wedge e_2 + bd \underbrace{e_2 \wedge e_2}_{=0}\) which when simplified is just \((ad-bc) e_1 \wedge e_2\).

(a3) This is just one specific example in the textbook; it doesn’t represent the general case (i.e., 1-forms do not always have to be unit length, nor does a collection of 1-forms always have to be orthonormal).

(a4) Antisymmetry holds for all k-vectors, whether basis vectors or not. For instance, it is true that \(e_i \wedge e_j = -e_j \wedge e_i\) for any pair of basis 1-vectors; it is also true that \(u \wedge v = -v \wedge u\) for any arbitrary pair of 1-vectors \(u,v\). (It might be useful for you to show that each of these statements implies the other, i.e., if the wedge on bases is antisymmetric then it is also antisymmetric for arbitrary vectors; likewise, if the wedge is antisymmetric for arbitrary vectors, it also is antisymmetric on basis vectors.)

Hi, I have a question about Hedge star. Consider an orthogonal basis {e1, e2} in R2. I wonder how did we get *e1 = e2. From the definition of Hedge star, we only have det(e1, *e1) = 1, which only says *e1(2) = 1 and is not enough to uniquely determine *e1. In class we use “e1 is orthogonal with *e1” to derive *e1(1) = 0. However, how is this “orthogonality” reflected in the computation of Hedge star? How to generalize it to k-vectors? Thanks in advance.

In the definition of the Hodge star, we always map a

basisto $k$-vector (e.g., $e_1 \wedge \cdots \wedge e_k$) to $\pm 1$ times a basis $(n-k)$-vector. The $\det(u, \star u) = 1$ constraint forces that the choice of Hodge star is unique. Does that answer your question?