What is the instantaneous velocity of an object moving in accordance to # f(t)= (t/(e^t+2t),t) # at # t=4 #?

Answer 1

The instantaneous velocity is #=(-0.0418,1)ms^-1#

We need

#(u/v)'=(u'v-uv')/(v^2)#
Start by calculating the derivative of #(t/(e^t+2t))# wrt #t#
#x=t/(e^t+2t)#
#u=t#, #=>#, #u'=1#
#v=e^t+2t#, #=>#, #v'=e^t+2#

So,

#dx/dt=(1*(e^t+2t)-t(e^t+2))/(e^t+2t)^2#
#=(e^t+2t-te^t-2t)/((e^t+2t)^2)#
#=(e^t-te^t)/((e^t+2t)^2)#
#=(e^t(1-t))/(e^t+2t)^2#

Also,

#y=t#
#dy/dt=1#

Therefore,

#v(t)=f'(t)= ((e^t(1-t))/(e^t+2t)^2,1)#
So, when #t=4#
#v(4)=f'(4)= ((e^4(1-4))/(e^4+2*4)^2,1)#
#=(-0.0418,1)#
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Answer 2

To find the instantaneous velocity of the object at (t = 4) when it is moving according to (f(t) = \left(\frac{t}{e^t + 2t}, t\right)), we need to find the derivative of the position function (f(t)) with respect to time (t). Then, evaluate the derivative at (t = 4) to obtain the instantaneous velocity vector. Let's denote the position function as (f(t) = (x(t), y(t))). Then, we can find the derivatives (x'(t)) and (y'(t)). After that, we substitute (t = 4) into these derivatives to find the velocities (v_x(4)) and (v_y(4)). Finally, we can express the instantaneous velocity vector as ((v_x(4), v_y(4))). Let's go through these steps.

  1. Find (x'(t)) and (y'(t)) using the quotient rule. [x'(t) = \frac{(e^t + 2t) - t(2e^t + 2)}{(e^t + 2t)^2}] [y'(t) = 1]

  2. Substitute (t = 4) into (x'(t)) and (y'(t)) to find (v_x(4)) and (v_y(4)). [x'(4) = \frac{(e^4 + 8) - 4(2e^4 + 2)}{(e^4 + 8)^2}] [y'(4) = 1]

  3. Calculate (v_x(4)) and (v_y(4)).

[v_x(4) = \frac{(e^4 + 8) - 4(2e^4 + 2)}{(e^4 + 8)^2}] [v_y(4) = 1]

  1. Express the instantaneous velocity vector at (t = 4) as ((v_x(4), v_y(4))).
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Answer from HIX Tutor

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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