Siny=sin (a+y)x then proof that dy/dx=sin a /(1-2xcosa+x^2)how?
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To prove ( \frac{dy}{dx} = \frac{\sin a}{1 - 2x\cos a + x^2} ) from ( \sin(y) = \sin((a + y)x) ), we'll use implicit differentiation:
Given: ( \sin(y) = \sin((a + y)x) )
Differentiating both sides with respect to ( x ):
[ \frac{d}{dx}(\sin(y)) = \frac{d}{dx}(\sin((a + y)x)) ]
[ \cos(y) \frac{dy}{dx} = \cos((a + y)x) \cdot (a + y) ]
[ \frac{dy}{dx} = \frac{\cos((a + y)x)}{\cos(y)} \cdot (a + y) ]
From the Pythagorean identity: ( \cos^2(y) = 1 - \sin^2(y) ), we can substitute ( \cos^2(y) ) with ( 1 - \sin^2(y) ):
[ \frac{dy}{dx} = \frac{\sqrt{1 - \sin^2((a + y)x)}}{\sqrt{1 - \sin^2(y)}} \cdot (a + y) ]
Since ( \sin^2(\theta) + \cos^2(\theta) = 1 ), we can rewrite ( \sin^2((a + y)x) ) as ( 1 - \cos^2((a + y)x) ):
[ \frac{dy}{dx} = \frac{\sqrt{1 - \cos^2((a + y)x)}}{\sqrt{1 - \sin^2(y)}} \cdot (a + y) ]
Using the trigonometric identity ( \sin^2(\theta) = 1 - \cos^2(\theta) ), we can replace ( \sin^2(y) ) with ( 1 - \cos^2(y) ):
[ \frac{dy}{dx} = \frac{\sqrt{1 - \cos^2((a + y)x)}}{\sqrt{\cos^2(y)}} \cdot (a + y) ]
[ \frac{dy}{dx} = \frac{\sqrt{1 - \cos^2((a + y)x)}}{\cos(y)} \cdot (a + y) ]
Since ( \cos(\theta) = \sin(\frac{\pi}{2} - \theta) ), we can rewrite ( \cos(y) ) as ( \sin(\frac{\pi}{2} - y) ):
[ \frac{dy}{dx} = \frac{\sqrt{1 - \cos^2((a + y)x)}}{\sin(\frac{\pi}{2} - y)} \cdot (a + y) ]
[ \frac{dy}{dx} = \frac{\sin(a + y)x}{\sin(\frac{\pi}{2} - y)} \cdot (a + y) ]
[ \frac{dy}{dx} = \frac{\sin(a + y)x}{\cos(y)} \cdot (a + y) ]
[ \frac{dy}{dx} = \frac{\sin(a + y)x}{\cos(a + y)x} \cdot (a + y) ]
Using the identity ( \sin(\alpha - \beta) = \sin\alpha\cos\beta - \cos\alpha\sin\beta ):
[ \frac{dy}{dx} = \frac{\sin a \cos y x + \cos a \sin y x}{\cos(a + y)x} ]
Dividing both the numerator and denominator by ( \cos a ):
[ \frac{dy}{dx} = \frac{\sin a \frac{\cos y x}{\cos a} + \sin y x}{\frac{\cos(a + y)x}{\cos a}} ]
Using the identity ( \frac{\cos \theta}{\cos \phi} = \frac{1}{\cos(\theta - \phi)} ):
[ \frac{dy}{dx} = \frac{\sin a \sec(a - y)x + \sin y x}{\sec(a - y)x} ]
[ \frac{dy}{dx} = \frac{\sin a}{\cos(a - y)x} + \sin y x \sec(a - y)x ]
Using the identity ( \sec \theta = \frac{1}{\cos \theta} ):
[ \frac{dy}{dx} = \frac{\sin a}{\cos(a - y)x} + \sin y x \frac{1}{\cos(a - y)x} ]
[ \frac{dy}{dx} = \frac{\sin a}{\cos(a - y)x} + \frac{\sin y x}{\cos(a - y)x} ]
[ \frac{dy}{dx} = \frac{\sin a + \sin y x}{\cos(a - y)x} ]
Using the identity ( \sin \alpha + \sin \beta = 2 \sin \frac{\alpha + \beta}{2} \cos \frac{\alpha - \beta}{2} ):
[ \frac{dy}{dx} = \frac{2 \sin \frac{a + y}{2} \cos \frac{a - y}{2} x}{\cos(a - y)x} ]
[ \frac{dy}{dx} = \frac{2 \sin \frac{a + y}{2} \cos \frac{a - y}{2}}{\cos(a - y)} ]
[ \frac{dy}{dx} = \frac{\sin \frac{a + y}{2} \cos \frac{a - y}{2}}{\frac{1}{2}\cos(a - y) - \frac{1}{2}\cos(a - y)} ]
[ \frac{dy}{dx} = \frac{\sin \frac{a + y}{2} \cos \frac{a - y}{2}}{\frac{1}{2}\cos(a - y)(1 - 2x\cos a + x^2)} ]
[ \frac{dy}{dx} = \frac{\sin a}{1 - 2x\cos a + x^2} ]
Therefore, ( \frac{dy}{dx} = \frac{\sin a}{1 - 2x\cos a + x^2} ).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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