The velocity of an object with a mass of #4 kg# is given by #v(t)= sin 3 t + cos 6 t #. What is the impulse applied to the object at #t= pi /3 #?
The impulse is
Then we have
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To find the impulse applied to the object at ( t = \frac{\pi}{3} ), we first need to find the velocity at that time by plugging ( t = \frac{\pi}{3} ) into the velocity equation. Then, we can find the change in momentum, which is equal to the impulse.
The velocity at ( t = \frac{\pi}{3} ) is: [ v\left(\frac{\pi}{3}\right) = \sin(3 \cdot \frac{\pi}{3}) + \cos(6 \cdot \frac{\pi}{3}) ] [ = \sin(\pi) + \cos(2\pi) ] [ = 0 + 1 = 1 ]
The impulse applied to the object at ( t = \frac{\pi}{3} ) is equal to the change in momentum. Since impulse is the integral of force with respect to time, and momentum is the integral of velocity with respect to time, impulse equals the change in momentum.
Since impulse ( J = \Delta p ), and momentum ( p = mv ) where ( m ) is mass and ( v ) is velocity, the impulse is ( J = mv - mu ).
Thus, the impulse applied to the object at ( t = \frac{\pi}{3} ) is ( J = m \cdot v\left(\frac{\pi}{3}\right) - m \cdot v(0) ), where ( v(0) ) is the initial velocity. Given that ( m = 4 ) kg and ( v(0) = v(0) = \sin(0) + \cos(0) = 0 + 1 = 1 ), we can calculate:
[ J = 4 \cdot 1 - 4 \cdot 1 = 0 ]
So, the impulse applied to the object at ( t = \frac{\pi}{3} ) is ( 0 ) Ns (Newtons seconds).
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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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