If # y = (sinx)^(sinx) # then find #dy/dx#?

Answer 1

#y'=sin(x)^sin(x)cos(x)*(ln(sin(x))+1)#

We want to find the derivative of

#y=(sin(x))^sin(x)#

Take the logarithm on both sides

#ln(y)=ln((sin(x))^sin(x))#
#ln(y)=sin(x)*ln(sin(x))#

Differentiate both sides using the product and chain rule

(Be aware of the implicit differentiation on the right side)

#y'*1/y=cos(x)ln(sin(x))+sin(x)cos(x)*1/sin(x)#
#y'=y*(cos(x)ln(sin(x))+sin(x)cos(x)*1/sin(x))#
#y'=y*(cos(x)ln(sin(x))+cos(x))#
#y'=y*cos(x)*(ln(sin(x))+1)#
Substitute #y=(sin(x))^sin(x)#
#y'=(sin(x))^sin(x)cos(x)*(ln(sin(x))+1)#
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Answer 2

#dy/dx= (sinx)^sinx (cosx+ cosx log sinx)#

#y= (sinx)^sinx # Taking log on both sides we get ,
#log y = sinx log sinx # Differentiating both sides we get ,
#1/y*dy/dx= sinx * 1/sinx *cosx+ cosx log sinx#or
#1/y*dy/dx= cancel(sinx) * 1/cancel(sinx) *cosx+ cosx log sinx# or
#dy/dx= y (cosx+ cosx log sinx)# or
#dy/dx= (sinx)^sinx (cosx+ cosx log sinx)# [Ans]
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Answer 3

#sin^sin(x)(x)(cos(x)lnsin(x)cos(x))#

We have to differentiate #sin(x)^sin(x)#.
Or maybe, #d/dxsin^sin(x)(x)#.
Remember, #a^b=e^(b*lna)#.
So the above becomes #d/dxe^(sin(x)*lnsin(x)#

Apply the chain rule:

The rule states that #(df(u))/dx=(df)/(du)*(du)/dx#.
Here, #f=e^u# and #u=sin(x)*lnsin(x)#

The equation simplifies (or gets excruciatingly confusing) to

#d/(du)e^u*d/dxsin(x)*lnsin(x)#
The derivative of #e^x# is #e^x#. So now the equation is:
#e^u*d/dxsin(x)*lnsin(x)#
Now for the second half. Remember the product rule: #(f*g)'=f'g+fg'#.

So now the equation is:

#e^u*d/dx(sin(x))*lnsin(x)+d/dx(lnsin(x))*sin(x)#
The derivative of #sin(x)# is #cos(x)#.
So the first derivative is #cos(x)lnsin(x)#. The equation is now #e^ucos(x)lnsin(x)*d/dx(lnsin(x))*sin(x)#
Sadly, we must use the chain rule again. Here, I take it as the differentiation of #f(w)#.
#f=lnw#, and #w=sin(x)#
The derivative of #lnw# is #1/w#, and #sin(x)# is again #cos(x)#
We now have #cos(x)/w#. But remember, #w=sin(x)#.
So this becomes #cos(x)/sin(x)#, which simplifies to #cot(x)#.
Our equation is presently #e^ucos(x)lnsin(x)cot(x)sin(x)#.
But #cot(x)sin(x)=cos(x)/sin(x)*sin(x)=cos(x)#
We now have #e^ucos(x)lnsin(x)cos(x)#. We're not done yet, though.
#u=sin(x)lnsin(x)#.
The equation is #e^(sin(x)lnsin(x))cos(x)lnsin(x)cos(x)#.
But #e^(b*lna)=a^b#.
So now, the equation is #sin^sin(x)(x)(cos(x)lnsin(x)cos(x))#

This, (thank God), cannot be simplified further.

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Answer 4

# dy/dx = cosx \ (sinx)^(sinx) \ {1+ ln sinx }#

We have:

# y = (sinx)^(sinx) #

If we take Natural Logarithms, we have:

# ln y = ln {(sinx)^(sinx) }#

And using the properties of logarithms we have:

# ln y = sinx \ ln sinx#
We can now readily differentiate wrt #x# by applying the chain rule (or implicit differentiation the LHS and the chain rule and the product rule on the RHS:
# 1/y \ dy/dx = (sinx)(1/sinx cosx) + (cosx)ln sinx #

Which we can simplify:

# 1/y \ dy/dx = cosx + cosx \ ln sinx #
# :. dy/dx = y{cosx + cosx \ ln sinx }# # \ \ \ \ \ \ \ \ \ \ = ycosx{1+ ln sinx }# # \ \ \ \ \ \ \ \ \ \ = cosx \ (sinx)^(sinx) \ {1+ ln sinx }#
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Answer 5

To find ( \frac{dy}{dx} ) for the given function ( y = (\sin x)^{\sin x} ), we will use logarithmic differentiation.

Taking natural logarithm on both sides: [ \ln y = \ln \left( (\sin x)^{\sin x} \right) ] [ \ln y = \sin x \cdot \ln(\sin x) ]

Now, differentiate implicitly with respect to ( x ): [ \frac{1}{y} \cdot \frac{dy}{dx} = \cos x \cdot \ln(\sin x) + \frac{\sin x}{\sin x} \cdot \frac{1}{\sin x} ] [ \frac{dy}{dx} = y \left( \cos x \cdot \ln(\sin x) + \cot x \right) ]

Substitute back ( y = (\sin x)^{\sin x} ) into the equation: [ \frac{dy}{dx} = (\sin x)^{\sin x} \left( \cos x \cdot \ln(\sin x) + \cot x \right) ]

Thus, ( \frac{dy}{dx} = (\sin x)^{\sin x} \left( \cos x \cdot \ln(\sin x) + \cot x \right) ).

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Answer from HIX Tutor

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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