What is the instantaneous velocity of an object moving in accordance to # f(t)= (sin2t-cos2t,sin(2t-pi/4)) # at # t=(-pi)/3 #?
And makes an angle with the positive direction of
and its direction can be given through the relation
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To find the instantaneous velocity of an object moving according to the function ( f(t) = (\sin(2t) - \cos(2t), \sin(2t - \frac{\pi}{4})) ) at ( t = -\frac{\pi}{3} ), we first need to differentiate the function with respect to ( t ) to find the velocity vector function. Then, we substitute ( t = -\frac{\pi}{3} ) into the velocity vector function to find the instantaneous velocity at that particular time.
Taking the derivative of ( f(t) ) with respect to ( t ), we get:
[ \frac{df}{dt} = \left( \frac{d}{dt}(\sin(2t) - \cos(2t)), \frac{d}{dt}(\sin(2t - \frac{\pi}{4})) \right) ]
Using the chain rule and the derivatives of sine and cosine functions, we get:
[ \frac{df}{dt} = (2\cos(2t) + 2\sin(2t), 2\cos(2t - \frac{\pi}{4})) ]
Now, substitute ( t = -\frac{\pi}{3} ) into the velocity vector function:
[ \frac{df}{dt}\bigg|_{t = -\frac{\pi}{3}} = (2\cos(-\frac{2\pi}{3}) + 2\sin(-\frac{2\pi}{3}), 2\cos(-\frac{2\pi}{3} - \frac{\pi}{4})) ]
Simplify the trigonometric functions:
[ \frac{df}{dt}\bigg|_{t = -\frac{\pi}{3}} = (-\sqrt{3} - 2, 2\cos(-\frac{11\pi}{12})) ]
Finally, compute the cosine value:
[ \cos(-\frac{11\pi}{12}) \approx -0.2588 ]
Therefore, the instantaneous velocity of the object at ( t = -\frac{\pi}{3} ) is approximately:
[ (-\sqrt{3} - 2, 2 \times (-0.2588)) ]
[ \approx (-2.732, -0.5176) ]
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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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