The problem involves analyzing the forces acting on a softball player during a head-first slide. Since the image is not displayed, we will consider the typical forces acting in this scenario without air resistance:
1. Gravitational force (weight) acting downwards. Denoted as \( F_g \) and is equal to \( m \times g \), where \( m \) is the mass of the player and \( g \) is the acceleration due to gravity.
2. Normal force acting upwards from the ground, opposite to the gravitational force. Denoted as \( F_N \) and typically equal in magnitude to \( F_g \) in a scenario without vertical acceleration. Thus, \( F_N = F_g \).
3. Frictional force acting opposite to the direction of the slide, which is to the left if the player is sliding to the right. The magnitude of the frictional force (\( F_f \)) depends on the coefficient of friction (\( \mu \)) between the player and the ground and the normal force. So, \( F_f = \mu \times F_N \).
There are no other forces acting in this scenario since we are ignoring air resistance. The relative magnitude of these forces will be (\( F_N = F_g \)) greater than \( F_f \), assuming a realistic coefficient of friction.
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