A bicyclist was moving at a rate of 5 m/s, and then sped up to 9 m/s. If the cyclist has a mass of 130 kg, how much work was needed to increase his velocity?

Answer 1

#3640J#

We know that KE#=1/2mv^2# ......(1)
Therefore, Change in KE, #Delta#KE#= 1/2 mv_f^2-1/2 mv_i^2# #=>Delta#KE#= 1/2 m(v_f^2-v_i^2)# ......(2) where #v_iand v_f# are initial and final velocities respectively of the cyclist.
Plug in all this information into the equation (2) #Delta#KE#= 1/2 xx130(9^2-5^2)# #=>Delta#KE#= 3640J#

Assuming that there are no losses, the change in kinetic energy is equal to the work done.

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Answer 2

The work needed to increase the velocity of the cyclist can be calculated using the work-energy principle. The change in kinetic energy is equal to the work done.

Initial kinetic energy (KE_1 = \frac{1}{2} mv_1^2)
Final kinetic energy (KE_2 = \frac{1}{2} mv_2^2)

Change in kinetic energy (ΔKE = KE_2 - KE_1)
Work done = (ΔKE)

Given:
Initial velocity (v_1 = 5 , \text{m/s})
Final velocity (v_2 = 9 , \text{m/s})
Mass of the cyclist (m = 130 , \text{kg})

Calculate (ΔKE = KE_2 - KE_1)
(KE_1 = \frac{1}{2} \times 130 \times (5)^2)
(KE_2 = \frac{1}{2} \times 130 \times (9)^2)

(ΔKE = \frac{1}{2} \times 130 \times (9)^2 - \frac{1}{2} \times 130 \times (5)^2)

(ΔKE = \frac{1}{2} \times 130 \times (81 - 25))

(ΔKE = \frac{1}{2} \times 130 \times 56)

(ΔKE = 3640 , \text{J})

Therefore, the work needed to increase the cyclist's velocity is (3640 , \text{J}).

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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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