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JUPITER SCIENCE

Derivative of cosθ using the First Principle

Derivative of \( cosθ \) using the First Principle

Let \(y\) = \( cosθ \)

∴ \(y + δy\) = \( cos(θ + δθ) \)

∴ \(δy\) = \( cos(θ + δθ) \) – \( cosθ \)
From Trigonometry , we have \( cos(A-B) \) = -2.\( sin \dfrac {(A+B)}{2} \).\( sin \dfrac {(A-B)}{2} \)
Using the above rule, we get
\(δy\) = -2.\( sin \dfrac {(θ+δθ + θ)}{2} \).\( sin \dfrac {(θ+δθ – θ)}{2} \)

or \(δy\) = -2\( sin (θ+ \dfrac{δθ}{2}) \) . \( sin( \dfrac {δθ}{2}) \)
∴ \(\dfrac {δy}{δθ}\) = -2 \( \dfrac { sin (θ+ \dfrac{δθ}{2}) sin( \dfrac {δθ}{2}) } {δθ}\)
or \(\dfrac {δy}{δθ}\) = -2 \(sin (θ+ \dfrac{δθ}{2}) \) \( \dfrac { sin( \dfrac {δθ}{2}) } {δθ}\)

∴ \(\dfrac {dy}{dx} = \) \( \lim_{δθ \to 0} \) (-2) . \(sin (θ+ \dfrac{δθ}{2}) \) \( \dfrac { sin( \dfrac {δθ}{2}) } {δθ} \)

= (-2) . \( \lim_{δθ \to 0} \) \(sin (θ+ \dfrac{δθ}{2}) \) . \( \lim_{δθ \to 0} \) \( \dfrac { sin( \dfrac {δθ}{2}) } {δθ} \)

= (-1).\( \lim_{δθ \to 0} \) \(sin (θ+ \dfrac{δθ}{2}) \) . \( \lim_{δθ \to 0} \) \( \dfrac { sin( \dfrac {δθ}{2}) } {\dfrac {δθ}{2}} \)

Also, from theorems on limits, we know that \( \lim_{x \to 0} \) \( \dfrac {sin(x)} {x} = 1\)

Thus we have
\(\dfrac {dy}{dx} = (-1). \) \( \lim_{δθ \to 0} \) \(sin (θ+ \dfrac{δθ}{2}) \) . \( \lim_{\dfrac {δθ}{2} \to 0} \) \( \dfrac { sin( \dfrac {δθ}{2}) } {(\dfrac {δθ}{2}) } \)

\(\dfrac {dy}{dx} = (-1).\) \(sin (θ+ 0) \) . 1 = \(-sinθ \)

 

Hence, \(\dfrac {d}{dx} \)\( (cosθ) \) = \( -sinθ \)

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