The velocity of an object with a mass of #6 kg# is given by #v(t)= sin 2 t + cos 4 t #. What is the impulse applied to the object at #t= (5pi)/12 #?
No answer to this
So we need a time period for there to be an impulse within the definition provided, and the Impulse is the change of momentum over that time period.
But that is the instantaneous momentum.
We can try
No luck :-(
The next port of call might be the Dirac delta function but I'm not sure where that might lead as it's been a while.
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To find the impulse applied to the object at ( t = \frac{5\pi}{12} ), we first need to find the velocity of the object at that time by substituting ( t = \frac{5\pi}{12} ) into the velocity equation:
( v\left(\frac{5\pi}{12}\right) = \sin(2 \cdot \frac{5\pi}{12}) + \cos(4 \cdot \frac{5\pi}{12}) )
( v\left(\frac{5\pi}{12}\right) = \sin\left(\frac{5\pi}{6}\right) + \cos\left(\frac{5\pi}{3}\right) )
( v\left(\frac{5\pi}{12}\right) = \sin\left(\frac{\pi}{6}\right) + \cos\left(\frac{\pi}{3}\right) )
( v\left(\frac{5\pi}{12}\right) = \frac{1}{2} + \frac{1}{2} )
( v\left(\frac{5\pi}{12}\right) = 1 )
The impulse applied to the object at ( t = \frac{5\pi}{12} ) is given by the change in momentum, which is the product of mass and change in velocity. Since impulse is a vector quantity, we need to consider the direction as well.
( \text{Impulse} = \Delta p = m \cdot \Delta v )
Since the object's mass ( m ) is given as 6 kg and the change in velocity ( \Delta v ) is ( 1 - 0 = 1 ), the impulse is ( 6 \times 1 = 6 , \text{kg m/s} ).
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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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