Using implicit differentiation on cosy=xcos(a+y), we treat y as a function of x, differentiate both sides, solve for dxdy, and simplify using the given relation to obtain dxdy=sinacos2(a+y).
The core idea here is implicit differentiation. The equation cosy=xcos(a+y) ties x and y together in a way that we cannot (and need not) solve for y explicitly. Instead, we differentiate both sides with respect to x, remembering that y is a function of x, so every time we hit a y, we multiply by dxdy (the chain rule). Then we isolate dxdy and use the original equation to simplify.
Let’s work through it step by step.
- Differentiate both sides with respect to x.
Left side: dxd[cosy]=−siny⋅dxdy.
Right side: dxd[xcos(a+y)]. This is a product: x times cos(a+y).
- Derivative of x is 1, so the first term: 1⋅cos(a+y)=cos(a+y).
- Derivative of cos(a+y) is −sin(a+y)⋅dxdy (chain rule again, since a is constant). Multiply by x: x⋅[−sin(a+y)dxdy]=−xsin(a+y)dxdy.
So the derivative of the right side is:
cos(a+y)−xsin(a+y)dxdy.
Putting it together:
−sinydxdy=cos(a+y)−xsin(a+y)dxdy.
- Collect all dxdy terms on one side.
Bring the term with dxdy from the right to the left:
−sinydxdy+xsin(a+y)dxdy=cos(a+y).
Factor out dxdy:
dxdy[−siny+xsin(a+y)]=cos(a+y).
- Solve for dxdy:
dxdy=−siny+xsin(a+y)cos(a+y).
This is a valid expression, but it still contains x and siny. We want it purely in terms of a and y. That’s where the original equation comes in.
- Use the original relation to eliminate x.
From cosy=xcos(a+y), we have:
x=cos(a+y)cosy.
Substitute this into the denominator:
−siny+xsin(a+y)=−siny+cos(a+y)cosy⋅sin(a+y).
Combine into a single fraction:
=cos(a+y)−sinycos(a+y)+cosysin(a+y).
Notice the numerator: −sinycos(a+y)+cosysin(a+y). This is exactly sin(a+y−y)? Let’s check: …