An object of mass 10 kg is moving with a velocity of 5 ms -1 . If the velocity of the object is tripled, the change in kinetic energy of the object is:
800%
This question asks us to find the percentage increase in the kinetic energy of an object when its velocity is tripled. We need to use the formula for kinetic energy and calculate the initial and final values to determine the change.
Kinetic energy (KE) is the energy an object possesses due to its motion. The formula for kinetic energy is given by:
$$ KE = \frac{1}{2}mv^2 $$
Where:
Mass ($m$) = 10 kg
Initial Velocity ($v_1$) = 5 m/s
Using the formula $KE = \frac{1}{2}mv^2$:
$$ KE_1 = \frac{1}{2} \times (10 \text{ kg}) \times (5 \text{ m/s})^2 $$
$$ KE_1 = \frac{1}{2} \times 10 \times 25 $$
$$ KE_1 = 5 \times 25 $$
$$ KE_1 = 125 \text{ Joules} $$
The velocity of the object is tripled. So, the new velocity ($v_2$) is:
$$ v_2 = 3 \times v_1 $$
$$ v_2 = 3 \times 5 \text{ m/s} $$
$$ v_2 = 15 \text{ m/s} $$
The mass remains the same: $m = 10$ kg.
Using the formula $KE = \frac{1}{2}mv^2$ with the new velocity:
$$ KE_2 = \frac{1}{2} \times (10 \text{ kg}) \times (15 \text{ m/s})^2 $$
$$ KE_2 = \frac{1}{2} \times 10 \times 225 $$
$$ KE_2 = 5 \times 225 $$
$$ KE_2 = 1125 \text{ Joules} $$
The change in kinetic energy is the difference between the final and initial kinetic energy:
$$ \Delta KE = KE_2 - KE_1 $$
$$ \Delta KE = 1125 \text{ J} - 125 \text{ J} $$
$$ \Delta KE = 1000 \text{ Joules} $$
The percentage change is calculated as:
$$ \text{Percentage Change} = \frac{\text{Change in KE}}{\text{Initial KE}} \times 100\% $$
$$ \text{Percentage Change} = \frac{\Delta KE}{KE_1} \times 100\% $$
$$ \text{Percentage Change} = \frac{1000 \text{ J}}{125 \text{ J}} \times 100\% $$
$$ \text{Percentage Change} = 8 \times 100\% $$
$$ \text{Percentage Change} = 800\% $$
When the velocity of the object is tripled, the kinetic energy increases significantly because it depends on the square of the velocity. The calculation shows that the change in kinetic energy is an increase of 800%.
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