Show that Dot-Product is Distributive

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The discussion revolves around proving the distributive property of the dot product using the definition \(\vec{A} \cdot \vec{B} = AB \cos \theta\). The original poster is attempting to show this property for three coplanar vectors without relying on components, expressing confusion about the correct application of angles and relationships between the vectors. Participants suggest using geometric relationships and the law of cosines to express angles and magnitudes, while emphasizing the need to avoid component-based definitions. The conversation highlights the challenge of maintaining clarity in vector relationships and angles when proving the distributive property without components. Overall, the thread illustrates the complexities involved in vector mathematics and the importance of precise definitions and geometric interpretations.
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PLEASE Skip to post #14 after reading problem statement; I am trying to solve this without using components

Homework Statement


Griffith's E&M problem 1.1. I feel good about my life.

Using the definition \vec{A}\cdot\vec{B} =AB\cos\theta show that the dot product is distributive when

(a) the 3 vectors are coplanar
(b)the general case
Okay then for part (a) I have started like this:

Let A B & C be 3 coplanar vectors. Let \theta be the angle between A & B; let \phi be between B & C and let \alpha be between A & C

then

\vec{A}\cdot(\vec{B}+\vec{C})=|\vec{A}||\vec{B+C}|\cos\gamma

where gamma is the angle between A and (B+C)

...now I am a little confused, i want to write that this implies

\vec{A}\cdot(\vec{B}+\vec{C})=(AB+AC)\cos\gamma

but I am not sure if that is correct. And if it is, where to go from here?
 
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I also drew this and came up with the four relationships seen in the box. I am not sure if this helps me :smile:
Picture1-30.png
 
Let \vec{A} = (a_x,a_y) etc. What is \vec{A} \cdot \vec{B} in terms of a_x, a_y, b_x and b_y?
 
I thought of using components, but the problem specifically asks to use the definition provided.

<br /> \vec{A}\cdot\vec{B} =AB\cos\theta
 
Well the intermediate step would rely on the definition. Plus it's easy to generalize.
 
qntty said:
Let \vec{A} = (a_x,a_y) etc. What is \vec{A} \cdot \vec{B} in terms of a_x, a_y, b_x and b_y?
\vec{A} \cdot \vec{B}=(a_xb_x+a_yb_y)

\Rightarrow (\vec{A} \cdot \vec{B})\cdot\vec{C}=(a_xb_xc_x+a_yb_yc_x)

Right?
 
Not sure what this intermediate step is? I could do the same for \vec{A} \cdot (\vec{B}\cdot\vec{C}) and show that they are equal w/out using the definition
 
Saladsamurai said:
(\vec{A} \cdot \vec{B})\cdot\vec{C}

Don't you mean (\vec{A} + \vec{B})\cdot\vec{C}?:confused:
 
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Saladsamurai said:
Not sure what this intermediate step is? I could do the same for \vec{A} \cdot (\vec{B}\cdot\vec{C}) and show that they are equal w/out using the definition

The intermediate step is to say that \vec{A} \cdot \vec{B}=(a_xb_x+a_yb_y) which is easier to work with in this case. You don't need to say \vec{A} \cdot (\vec{B}\cdot\vec{C}) is equal to anything and in fact you can't because the dot product is only for vectors.
 
  • #10
qntty said:
Don't you mean (\vec{A} + \vec{B})\cdot\vec{C}?:confused:

Sorry, I was working on another problem at the same time :smile:

One minute...
 
  • #11
okay...I still don't see how this:

(\vec{A} + \vec{B})\cdot\vec{C}=(a_x+b_x)c_x+(a_y+b_y)c_y=a_xc_x+b_xc_x+a_yc_y+b_yc_y=\vec{A}\cdot\vec{B}+\vec{B}\cdot\vec{C}

uses the definition of dot-product \vec{A}\cdot\vec{B} =AB\cos\theta

Sorry :confused:
 
  • #12
To prove that

\vec{A}\cdot\vec{B}=a_xb_x+a_yb_y

you have to use the definition. If the angle of \vec{A} is \alpha and the angle of \vec{B} is \beta then\vec{A}\cdot\vec{B} = |\vec{A}||\vec{B}|\cos{(\alpha-\beta)}

=|\vec{A}||\vec{B}|(\cos{\alpha}\cos{\beta}+sin{\alpha}\sin{\beta})

=|\vec{A}|\cos{\alpha}|\vec{B}|\cos\beta+|\vec{A}|sin{\alpha}|\vec{B}|\sin{\beta}

=a_xb_x+a_yb_y
 
  • #13
This is an interesting approach. Thanks qntty!

The only thing is that the question is asked (in the text) before the component-wise definition of the Dot-Product is even given.

This leads me to wonder if there is a way to show that the dot-product is distributive without ever going into components.

I think that my original approach might lead somewhere. You have given me an idea to modify it though. I like how you used an absolute reference frame when naming your angles, instead of the way I named them (i.e., wrt the vectors themselves).

I will play around with this a little, but it is really difficult for me to see a way to do this w/out components coming into play.

Thanks again :smile:
 
  • #14
Okay, scratch that last post. I am going to stick with my original way of labeling angles (i.e., wrt the vectors themselves, not the reference frame)

Here is my new diagram:

Picture3-13.png


Now, since I already know that the dot product distributes then I know that I am shooting for

(\vec{A} + \vec{B})\cdot\vec{C}=\vec{A}\cdot\vec{B}+\vec{ B}\cdot\vec{C}

So the end result should be

something=|A||B|\cos\beta+|B||C|\cos\gamma

From my diagram I have

(\vec{A} + \vec{B})\cdot\vec{C}=|A||B+C|\cos\phi

This leads me to believe that I must write \phi in terms of \beta and \gammaFrom my diagram, I also have the relationships:

\phi=\beta+s
\phi=(\beta+\gamma)-r

Beta and gamma are 'known' and r, s, and phi are unknown...

Seems like I am one equation short of doing something. :smile:

Any ideas?
 
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  • #15
Hint: |\vec{B}+\vec{C}|=___?
 
  • #16
gabbagabbahey said:
Hint: |\vec{B}+\vec{C}|=___?

I don't know without using components :confused:
 
  • #17
Saladsamurai said:
I don't know without using components :confused:

Try drawing the tail of the vector C at the head of the vector B and draw in the vector B+C. Draw all the angles in and use the law of cosines.
 
  • #18
gabbagabbahey said:
Try drawing the tail of the vector C at the head of the vector B and draw in the vector B+C. Draw all the angles in and use the law of cosines.

If I do it this way, I think that I will need to go back to defining the angle wrt a datum instead of from vector to vector... other wise, i do not know what angles to write in.
 
  • #19
Extend a dotted line along the direction of B and label \gamma the same way as before...you should quickly see that one of the angles in your triangle is \pi-\gamma:wink:
 
  • #20
Photo1-2.jpg
Hmmm. I don't see how an angle inside my triangle is pi-gamma.

Maybe I'm cooked ...
 
  • #21
What if I drop a perpendicular from the tip of C to my extension of B.. then wouldn't the angle between B+C and C just be gamma?
 
  • #22
Basic Trig...look at the large angle adjacent to gamma...if gamma were zero you would simply have a straight line (pointing in the direction of B) and that angle would be 180 degrees or pi radians, in general that angle is (180 deg- gamma)
 
  • #23
Saladsamurai said:
What if I drop a perpendicular from the tip of C to my extension of B.. then wouldn't the angle between B+C and C just be gamma?

No, because B+C is not parallel to B
 
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  • #24
gabbagabbahey said:
Basic Trig...look at the large angle adjacent to gamma...if gamma were zero you would simply have a straight line (pointing in the direction of B) and that angle would be 180 degrees or pi radians, in general that angle is (180 deg- gamma)

Oh man :blushing: When I read your post, you said pi - gamma, but I was thinking pi/2 - gamma...pi = 180 ... my brain = pudding
 
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