What is #f(x) = int tanx-secx dx# if #f(pi/4)=-1 #?

Answer 1

#f(x)=-ln|cosx|-ln|secx+tanx|-ln(sqrt2/(sqrt2+1))-1#

As #inttanxdx=-ln|cosx|# and #intsecxdx=ln|secx+tanx|#
#f(x)=int(tanx-secx)dx#
= #-ln|cosx|-ln|secx+tanx|+c#
Hence #f(pi/4)=-ln|1/sqrt2|-ln|sqrt2+1|+c=-1#
or #ln(sqrt2)-ln(sqrt2+1)+c=-1#
or #ln(sqrt2/(sqrt2+1))+c=-1#
or #c=-ln(sqrt2/(sqrt2+1)))-1#
and #f(x)=int(tanx-secx)dx#
= #-ln|cosx|-ln|secx+tanx|-ln(sqrt2/(sqrt2+1))-1#
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Answer 2

To find ( f(x) = \int \tan(x) - \sec(x) , dx ) if ( f(\frac{\pi}{4}) = -1 ), we need to first integrate the given function.

( \int \tan(x) - \sec(x) , dx = \int \tan(x) , dx - \int \sec(x) , dx )

The antiderivative of ( \tan(x) ) is ( -\ln|\cos(x)| ) and the antiderivative of ( \sec(x) ) is ( \ln|\sec(x) + \tan(x)| ).

So, ( f(x) = -\ln|\cos(x)| - \ln|\sec(x) + \tan(x)| + C ), where ( C ) is the constant of integration.

Given ( f(\frac{\pi}{4}) = -1 ), we substitute ( x = \frac{\pi}{4} ) into the function:

( -1 = -\ln|\cos(\frac{\pi}{4})| - \ln|\sec(\frac{\pi}{4}) + \tan(\frac{\pi}{4})| + C )

( -1 = -\ln|\frac{1}{\sqrt{2}}| - \ln|\frac{1+\sqrt{2}}{\sqrt{2}}| + C )

( -1 = -\ln\left(\frac{1}{\sqrt{2}}\right) - \ln\left(\frac{1+\sqrt{2}}{\sqrt{2}}\right) + C )

( -1 = -\ln(1) + \frac{1}{2}\ln(2) - \ln(1+\sqrt{2}) + C )

( -1 = \frac{1}{2}\ln(2) - \ln(1+\sqrt{2}) + C )

Now, we solve for ( C ):

( C = -1 - \frac{1}{2}\ln(2) + \ln(1+\sqrt{2}) )

Thus, the function ( f(x) = \int \tan(x) - \sec(x) , dx ) with ( f(\frac{\pi}{4}) = -1 ) is:

( f(x) = -\ln|\cos(x)| - \ln|\sec(x) + \tan(x)| - 1 - \frac{1}{2}\ln(2) + \ln(1+\sqrt{2}) )

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Answer 3

To find ( f(x) = \int \tan(x) - \sec(x) , dx ) when ( f\left(\frac{\pi}{4}\right) = -1 ), we first need to find the antiderivative of ( \tan(x) - \sec(x) ) and then evaluate it at ( x = \frac{\pi}{4} ).

The antiderivative of ( \tan(x) ) is ( -\ln|\cos(x)| ), and the antiderivative of ( \sec(x) ) is ( \ln|\sec(x) + \tan(x)| ).

So, the antiderivative of ( \tan(x) - \sec(x) ) is ( -\ln|\cos(x)| - \ln|\sec(x) + \tan(x)| ).

We need to evaluate this antiderivative at ( x = \frac{\pi}{4} ):

( f\left(\frac{\pi}{4}\right) = -\ln|\cos\left(\frac{\pi}{4}\right)| - \ln|\sec\left(\frac{\pi}{4}\right) + \tan\left(\frac{\pi}{4}\right)| )

Now, ( \cos\left(\frac{\pi}{4}\right) = \frac{1}{\sqrt{2}} ), ( \sec\left(\frac{\pi}{4}\right) = \sqrt{2} ), and ( \tan\left(\frac{\pi}{4}\right) = 1 ).

So, ( f\left(\frac{\pi}{4}\right) = -\ln\left|\frac{1}{\sqrt{2}}\right| - \ln\left|\sqrt{2} + 1\right| )

Simplify:

( f\left(\frac{\pi}{4}\right) = -\ln\left(\frac{1}{\sqrt{2}}\right) - \ln\left(\sqrt{2} + 1\right) )

Now, recall that ( \ln\left(\frac{1}{a}\right) = -\ln(a) ).

So, ( f\left(\frac{\pi}{4}\right) = \ln(\sqrt{2}) - \ln(\sqrt{2} + 1) )

( f\left(\frac{\pi}{4}\right) = \ln\left(\frac{\sqrt{2}}{\sqrt{2} + 1}\right) )

Given that ( f\left(\frac{\pi}{4}\right) = -1 ), we have:

( \ln\left(\frac{\sqrt{2}}{\sqrt{2} + 1}\right) = -1 )

Taking the exponential of both sides to solve for the fraction:

( e^{-1} = \frac{\sqrt{2}}{\sqrt{2} + 1} )

Solve for the fraction:

( e^{-1}(\sqrt{2} + 1) = \sqrt{2} )

( e^{-1}\sqrt{2} + e^{-1} = \sqrt{2} )

( e^{-1}\sqrt{2} = \sqrt{2} - e^{-1} )

Divide both sides by ( \sqrt{2} ):

( e^{-1} = \frac{\sqrt{2} - e^{-1}}{\sqrt{2}} )

( e^{-1} = \frac{\sqrt{2}}{\sqrt{2}} - \frac{e^{-1}}{\sqrt{2}} )

( e^{-1} = 1 - \frac{e^{-1}}{\sqrt{2}} )

Add ( \frac{e^{-1}}{\sqrt{2}} ) to both sides:

( e^{-1} + \frac{e^{-1}}{\sqrt{2}} = 1 )

Factor out ( e^{-1} ):

( e^{-1}(1 + \frac{1}{\sqrt{2}}) = 1 )

Now, we solve for ( e^{-1} ):

( e^{-1} = \frac{1}{1 + \frac{1}{\sqrt{2}}} )

Multiply the numerator and the denominator by ( \sqrt{2} ):

( e^{-1} = \frac{\sqrt{2}}{\sqrt{2} + 1} )

Compare this result to the previous expression for ( e^{-1} ):

( e^{-1} = \frac{\sqrt{2}}{\sqrt{2} + 1} )

Therefore, we've verified that ( e^{-1} = \frac{\sqrt{2}}{\sqrt{2} + 1} ).

Hence, ( f\left(\frac{\pi}{4}\right) = -1 ).

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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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