A high jumper approaches the bar at \(9.0 \mathrm{~m} / \mathrm{s}\). What is the highest altitude the jumper can reach, if he does not use any additional push off the ground and is moving at \(7.0 \mathrm{~m} / \mathrm{s}\) as he goes over the bar?

Kinetic energy is the energy that an object possesses due to its motion. It's an important concept in physics because it quantifies the amount of work that a moving object can perform due to its velocity. The formula for kinetic energy (\textbf{KE}) is given by \( KE = \frac{1}{2}mv^2 \), where \( m \) is the mass of the object and \( v \) is its velocity.

In the context of our high jumper problem, we can see kinetic energy in action as the jumper moves towards the bar. As the velocity of the jumper changes, so does his kinetic energy. This is crucial, because, upon taking off from the ground, some of the kinetic energy is converted to potential energy, allowing the jumper to reach a certain height.

Potential energy is the energy stored in an object due to its position or arrangement. Gravitational potential energy, for instance, is energy that an object possesses because of its position in a gravitational field. The formula for gravitational potential energy (\textbf{PE}) is given by \( PE = mgh \), where \( m \) is the mass, \( g \) is the acceleration due to gravity (\( 9.81 \text{m/s}^2 \) on Earth), and \( h \) is the height above the reference point.

For our high jumper, the highest altitude he can reach is determined by when all the kinetic energy, that isn’t lost to other forces, is converted to potential energy. The jumper's initial potential energy at ground level is zero which increases as he ascends.

The principle of conservation of mechanical energy states that the total mechanical energy of an isolated system remains constant as long as only conservative forces, like gravity, are acting on it. Mechanical energy is the sum of kinetic and potential energy. This principle can be written as \( KE_{i} + PE_{i} = KE_{f} + PE_{f} \), with ‘i’ indicating initial and ‘f’ indicating final states. Non-conservative forces, like friction or air resistance, can cause this energy to change, but they are ignored in ideal scenarios.

In the given exercise, by setting the initial potential energy on the ground to zero and considering no other forces but gravity, we applied energy conservation to solve for the maximum height the jumper could reach. The equation \( K_f + U_f = K_i + U_i \) captures the energy transformation from kinetic to potential, allowing us to predict how high the jumper will go.

Kinematics is the branch of mechanics that describes the motion of points, objects, and systems without considering the forces that cause them to move. It focuses on displacement, velocity, acceleration, and time. These concepts are fundamental when analyzing the motion of objects, as they help understand trajectories and motion patterns without delving into what actually propels or alters that motion.

Relating to our jumper, kinematics would not only look at the jumper's speeds at various points but could extend to the trajectory he takes throughout his jump. Even though our problem didn’t require a deep dive into kinematics, understanding how motion is described in physics provides a foundation for more complex problems where kinematics and energy conservation intertwine.