How do you find the equation of the tangent line to the curve #y=2xsinx# at #(pi/2,pi)#?
The equation of the tangent is
I thought it would be easier to make a little video rather than try and write out my explanation.
I hope it helps :)
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To find the equation of the tangent line to the curve y=2xsinx at the point (pi/2, pi), we need to find the slope of the tangent line and then use the point-slope form of a linear equation.
To find the slope of the tangent line, we can use the derivative of the function y=2xsinx. Taking the derivative of y with respect to x, we get:
dy/dx = 2sinx + 2xcosx
Now, substitute the x-coordinate of the given point (pi/2) into the derivative to find the slope at that point:
dy/dx = 2sin(pi/2) + 2(pi/2)cos(pi/2) = 2(1) + 2(pi/2)(0) = 2
So, the slope of the tangent line at (pi/2, pi) is 2.
Using the point-slope form of a linear equation, we can write the equation of the tangent line:
y - y1 = m(x - x1)
Substituting the values of the point (pi/2, pi) and the slope (2) into the equation, we get:
y - pi = 2(x - pi/2)
Simplifying the equation, we have:
y = 2x - pi + 2(pi/2) y = 2x - pi + pi y = 2x
Therefore, the equation of the tangent line to the curve y=2xsinx at the point (pi/2, pi) is y = 2x.
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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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