How do you use the first part of the Fundamental Theorem of Calculus to find the derivative of #y = int 3(sin(t))^4 dt# from #e^x# to 1?
The derivative is
Recall that the antiderivative of a function can be used to calculate the definite integral of that function according to the calculus fundamental theorem.
Likewise:
We take the derivative because the question requests it.
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To find the derivative of ( y = \int_{e^x}^1 3(\sin(t))^4 , dt ) using the first part of the Fundamental Theorem of Calculus, we first need to express the integral as a function of ( x ). We'll let ( F(x) ) be the antiderivative of ( 3(\sin(t))^4 ) with respect to ( t ). Then, by the Fundamental Theorem of Calculus, the integral ( \int_{e^x}^1 3(\sin(t))^4 , dt ) is equal to ( F(1) - F(e^x) ).
To find ( F(x) ), we need to find the antiderivative of ( 3(\sin(t))^4 ) with respect to ( t ). This involves using trigonometric identities and integration techniques. After finding ( F(x) ), we evaluate ( F(1) ) and ( F(e^x) ), and then take the difference.
Finally, to find the derivative of ( y ) with respect to ( x ), we differentiate ( F(1) - F(e^x) ) using the chain rule, which states that if ( F(x) ) is differentiable at ( x ) and ( g(x) ) is differentiable at ( x ), then ( F(g(x)) ) is differentiable at ( x ) and ( (F(g(x)))' = F'(g(x)) \cdot g'(x) ). We compute ( \frac{d}{dx}[F(1) - F(e^x)] ) accordingly.
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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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