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Question: A. In a unit vector notation, what is \[\vec r = \vec a - \vec b + \vec c\]when \[\vec a = 5\hat i +...

A. In a unit vector notation, what is r=ab+c\vec r = \vec a - \vec b + \vec cwhen a=5i^+4k^\vec a = 5\hat i + 4\hat k, b=2i^+2j^+3k^\vec b = - 2\hat i + 2\hat j + 3\hat k and c=4i^+3j^+2k^\vec c = 4\hat i + 3\hat j + 2\hat k,
B. Calculate the angle between r\vec rand the positive – axis.
C. What is the component of a\vec a along the direction of b\vec b
D. What is the perpendicular to the direction of b\vec b but in the plane of b\vec b and a\vec a?

Explanation

Solution

To answer this question we will first define what is a unit vector. Next step is to answer each part of this question with a detailed explanation. We will first find answer A by substituting values of , a\vec a, b\vec band c\vec cin r\vec rand then finding the unit vector using its formula. For part b and c and d there are direct formulas available, hence we will simply apply those formulas and solve the questions.

Formula Used:
Unit vector= u^=uu\hat u = \dfrac{u}{{|u|}} where u is a vector.
Angle between vectors:
cosθ=a.bab\cos \theta = \dfrac{{\vec a.\vec b}}{{\left| {\vec a} \right|\left| {\vec b} \right|}} where a and b are given vectors.
For component of a\vec a perpendicular to b\vec b In the plane of a\vec a and b\vec b we use: a×(b×a)a2\dfrac{{\vec a \times \left( {\vec b \times \vec a} \right)}}{{{{\left| a \right|}^2}}}

Complete step by step solution:
Let us first know what a unit vector is: it is such a vector whose magnitude is one.
Let us answer question A.
A. It has been given that: a=5i^+4k^\vec a = 5\hat i + 4\hat k, b=2i^+2j^+3k^\vec b = - 2\hat i + 2\hat j + 3\hat k and c=4i^+3j^+2k^\vec c = 4\hat i + 3\hat j + 2\hat k,
We have to find r\vec rwhich is r=ab+c\vec r = \vec a - \vec b + \vec c.
Let us substitute the values of , a\vec a, b\vec band c\vec cin r\vec r
We get : r=5i^+4k^(2i^+2j^+3k^)+4i^+3j^+2k^\vec r = 5\hat i + 4\hat k - \left( { - 2\hat i + 2\hat j + 3\hat k} \right) + 4\hat i + 3\hat j + 2\hat k
Or, r=5i^+4k^+2i^2j^3k^+4i^+3j^+2k^\vec r = 5\hat i + 4\hat k + 2\hat i - 2\hat j - 3\hat k + 4\hat i + 3\hat j + 2\hat k
Or, r=5i^+2i^+4i^2j^+3j^3k^+2k^+4k^\vec r = 5\hat i + 2\hat i + 4\hat i - 2\hat j + 3\hat j - 3\hat k + 2\hat k + 4\hat k
Or, r=(5+2+4)i^+(32)j^+(3+2+4)k^\vec r = \left( {5 + 2 + 4} \right)\hat i + \left( {3 - 2} \right)\hat j + \left( { - 3 + 2 + 4} \right)\hat k
Or, r=11i^+1j^+3k^\vec r = 11\hat i + 1\hat j + 3\hat k
Hence for unit vector notation we have to use: r^=rr\hat r = \dfrac{r}{{|r|}}
Lets find r|r|.
r=112+12+32|r| = \sqrt {{{11}^2} + {1^2} + {3^2}}
Or, r=121+1+9|r| = \sqrt {121 + 1 + 9}
Or, r=131|r| = \sqrt {131}
Hence the answer A is : r^=rr\hat r = \dfrac{r}{{|r|}}= r^=11i^+1j^+3k^131\hat r = \dfrac{{11\hat i + 1\hat j + 3\hat k}}{{\sqrt {131} }},
B. Now we know that r=11i^+1j^+3k^\vec r = 11\hat i + 1\hat j + 3\hat k hence the angle of this with z-axis is given by
cosθ=a.bab\cos \theta = \dfrac{{\vec a.\vec b}}{{\left| {\vec a} \right|\left| {\vec b} \right|}}
or, cosθ=r.k^rk^\cos \theta = \dfrac{{\vec r.\hat k}}{{\left| {\vec r} \right|\left| {\hat k} \right|}}
Or, cosθ=(11i^+1j^+3k^)k^131×1\cos \theta = \dfrac{{\left( {11\hat i + 1\hat j + 3\hat k} \right)\hat k}}{{\sqrt {131} \times \sqrt 1 }}
Or, cosθ=0i^+0j^+3k^131\cos \theta = \dfrac{{0\hat i + 0\hat j + 3\hat k}}{{\sqrt {131} }} (k^×i^=k^×j^=0)\left( {\because \hat k \times \hat i = \hat k \times \hat j = 0} \right)and (k^×k^=1)\left( {\because \hat k \times \hat k = 1} \right)
Or, cosθ=3k^131\cos \theta = \dfrac{{3\hat k}}{{\sqrt {131} }}.
Hence angle θ=cos15131\theta = {\cos ^{ - 1}}\dfrac{5}{{\sqrt {131} }}.
C. Here the component of a\vec a along b\vec b is a.bb\dfrac{{\vec a.\vec b}}{{\left| {\vec b} \right|}}
Hence projection is (5i^+4k^).(2i^+2j^+3k^)2i^2j^3k^\dfrac{{\left( {5\hat i + 4\hat k} \right).\left( { - 2\hat i + 2\hat j + 3\hat k} \right)}}{{\left| {2\hat i - 2\hat j - 3\hat k} \right|}}
Or, 10+0+1222+22+32\dfrac{{ - 10 + 0 + 12}}{{\sqrt {{2^2} + {2^2} + {3^2}} }}
Or, 24+4+9\dfrac{2}{{\sqrt {4 + 4 + 9} }}
Or, 217\dfrac{2}{{\sqrt {17} }}.
D. For the perpendicular to the direction of b\vec b but in the plane of b\vec b and a\vec a:
a2b2\sqrt {{{\left| a \right|}^2} - {{\left| b \right|}^2}}
or, 52+42(2)2172\sqrt {{5^2} + {4^2} - \dfrac{{{{\left( 2 \right)}^2}}}{{{{\sqrt {17} }^2}}}} (we have already found the value for b\left| b \right|).
Or, 25+16417\sqrt {25 + 16 - \dfrac{4}{{17}}}
Or, 41417\sqrt {41 - \dfrac{4}{{17}}}
Or, 697417\sqrt {\dfrac{{697 - 4}}{{17}}}
Or, 69317\sqrt {\dfrac{{693}}{{17}}} .

Note:
In the first part, remember to check the answer, find if the answer that we have found is a unit vector or no. to check this we have to find the magnitude of r\vec r. That is we will find r^=rr\left| {\hat r = \dfrac{r}{{|r|}}} \right|,
We will see that its magnitude comes out to be 1. Hence our answer is correct.
In the 2nd question, remember to use the formula for angle using cosθ\cos \theta and not sinθ\sin \theta . We have to use this because a.b=abcosθ\vec a.\vec b = \left| {\vec a} \right|\left| {\vec b} \right|\cos \theta is used to find angles between them.