Grade 11 Basic Mathematics by Sukunda Pustak Vawan Notes and Solutions | Nepal
Disclaimer:
1. A force equal to 10 N is inclined at an angle of 30 to the horizontal;
find its resolved parts in a horizontal and vertical directions.
Solution:
Let F = 10 N
\theta = 30^o
We know,
Horizontal component F_x= F cos \theta
= 10 * cos 30
= 10 \times \dfrac{\sqrt{3}}{2}
= 5 \sqrt{3} N
Vertical component F_y = F sin \theta
= 10 * sin 30
= 10 * \dfrac{1}{2}
= 5 N
2. Resolve a force equal to 50 N into two forces making angles of 60 and 45 with it in opposite sides.
Solution:
Let the two resolved forces be A and B and their angles with the original force be denoted by \alpha and \beta, respectively.
Then, we have,
A = \dfrac{50 \sin \alpha}{sin( \alpha + \beta)}
= \dfrac{50 \sin 60^o}{\sin (60 + 45)}
= \dfrac{50 \times \frac{ \sqrt{3}}{2} }{ \sin 105^o}
= \dfrac{25 \sqrt{3}}{ \frac{ \sqrt{3} + 1}{2 \sqrt{2}}}
= \dfrac{25 \sqrt{3} \times 2 \sqrt{2}}{\sqrt{3} + 1}
= \dfrac{50 \sqrt{6} }{ \sqrt{3} + 1} \times \dfrac{ \sqrt{3} - 1}{ \sqrt{3} -1 }
= \dfrac{50 \sqrt{6} ( \sqrt{3} - 1)}{3 - 1}
= 25 (3 \sqrt{2} - \sqrt{6}) N
And
A = \dfrac{50 \sin \alpha}{sin( \alpha + \beta)}
= \dfrac{50 \sin 45^o}{\sin (60 + 45)}
= \dfrac{50 \times \frac{ 1}{\sqrt{2}} }{ \sin 105^o}
= \dfrac{25 \sqrt{2}}{ \frac{ \sqrt{3} + 1}{2 \sqrt{2}}}
= \dfrac{25 \sqrt{2} \times 2 \sqrt{2}}{\sqrt{3} + 1}
= \dfrac{50 \times 2}{\sqrt{3} + 1} \times \dfrac{\sqrt{3} - 1}{\sqrt{3} - 1}
= \dfrac{100 (\sqrt{3} -1)}{3 -1}
= 50(\sqrt{3}-1) N
Hence, the required forces are $25 (3 \sqrt{2} - \sqrt{6})$ N and 50 ( \sqrt{3} -1 ) N.
3. If a force P be resolved into two forces making angles of 45 and 15 with
its direction; show that the latter force is \dfrac{\sqrt{6}}{3} P.
Solution:
Let the two resolved forces be respresented by A and B and their angle with the force P be \alpha and \beta.
Then,
A = \dfrac{P \sin \alpha}{sin(\alpha + \beta)}
A = \dfrac{P \sin 45^o}{sin(45+15)^o}
= \dfrac{P \times \dfrac{1}{\sqrt{2}}}{sin 60^o}
= \dfrac{P \times \dfrac{1}{\sqrt{2}}}{\dfrac{\sqrt{3}}{2}}
= \dfrac{P \times 2}{\sqrt{6}}
= \dfrac{P \times 2 }{\sqrt{6}} \times \dfrac{\sqrt{6}}{\sqrt{6}}
= \dfrac{P \times 2 \sqrt{6}}{6}
= \dfrac{\sqrt{6}}{3}P
However, the latter force is B that makes angle \beta with the given force. Just to make the answer matching with the book, we solved it accordingly.
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