Component of a vector along another vector.

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Homework Help Overview

The discussion revolves around finding the component of vector \(\vec{A}\) along vector \(\vec{B}\), with given vectors \(\vec{A}=2\hat{i}+3\hat{j}\) and \(\vec{B}=\hat{i}+\hat{j}\). Participants are exploring the mathematical relationships and formulas involved in vector projections.

Discussion Character

  • Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of the component of \(\vec{A}\) along \(\vec{B}\) using the dot product and the angle between the vectors. There are attempts to clarify the steps involved in the projection process, including the use of unit vectors.

Discussion Status

Some participants express disagreement with the textbook solution, suggesting that it may not accurately reflect the projection's dependence on direction rather than magnitude. There is an ongoing examination of the formulas used and their implications for the results.

Contextual Notes

Participants note potential discrepancies in the textbook's approach and the implications of dividing by the magnitude of \(\vec{B}\) multiple times. The discussion includes considerations of how cosine relates to the component of \(\vec{A}\) along \(\vec{B}\).

Hijaz Aslam
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Homework Statement


Given ##\vec{A}=2\hat{i}+3\hat{j}## and ##\vec{B}=\hat{i}+\hat{j}##.Find the component of ##\vec{A}## along ##\vec{B}##.

Homework Equations


##\vec{A}.\vec{B}=ABcosθ## where θ is the angle between both the vectors.

The Attempt at a Solution


I attempted the question as follows:
Let the angle between ##\vec{A}## and ##\vec{B}## be 'θ'. So the component of ##\vec{A}## along ##\vec{B}## is given by ##Acosθ\hat{B}## => ##Acosθ(\frac{\vec{B}}{B})##

As ##\vec{A}.\vec{B}=ABcosθ## => ##[( 2\hat{i}+3\hat{j})(\hat{i}+\hat{j})]/B=Acosθ## => ##\frac{5}{\sqrt{2}}=Acosθ##

Therefore the component is : ##\frac{5}{\sqrt{2}}(\frac{\hat{i}+\hat{j}}{\sqrt{2}})## => ##\frac{5}{2}({\hat{i}+\hat{j}})##

But my text produces the solution as follows:
##A_B=(\vec{A}.\vec{B})\hat{B}=\frac{5}{\sqrt{2}}(\hat{i}+\hat{j})##.
 
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Hijaz Aslam said:
Therefore the component is : ##\frac{5}{\sqrt{2}}(\frac{\hat{i}+\hat{j}}{\sqrt{2}})## => ##\frac{5}{2}({\hat{i}+\hat{j}})##

But my text produces the solution as follows:
##A_B=(\vec{A}.\vec{B})\hat{B}=\frac{5}{\sqrt{2}}(\hat{i}+\hat{j})##.

I usually see this process broken down into basis components.
That is ##\hat B =\sqrt{2}/2 \hat i + \sqrt{2}/2 \hat j. ##
Then the component is ##A\cdot \hat B_i \hat i + A\cdot \hat B_j \hat j ##.
Somewhere in your process, you divided by the magnitude of B twice.
 
Hijaz Aslam said:
But my text produces the solution as follows:
AB=(A⃗ .B⃗ )B^=52√(i^+j^)A_B=(\vec{A}.\vec{B})\hat{B}=\frac{5}{\sqrt{2}}(\hat{i}+\hat{j}).

You're right and the book is wrong. The book answer as well as the formula for AB they use.
The length of your answer is smaller than the length of A as it should be. The book answer is larger.
The projection of A on B should only depend on the direction of B, not the magnitude. The formula used for AB in the book does depend on the magnitude of B.
 
Book is wrong . We can verify this by standard euclidean geometry easily because by the definition of cosine, it will be cos(θ)=(component of A along B)/A hence Acos(θ)=(component of A along B). And we have to multiply this by the unit vector of B to get the required result.
 

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