When a spring is compressed against a wall, both the wall and the person exert forces on the spring, leading to its compression. However, the wall remains stationary while the person's hand moves, which simplifies the analysis to attribute the compression primarily to the person's action. The spring's compression is defined by the relationship F = -kx, where k is the spring constant and x is the change in length from its rest position. It is not possible to determine how much each hand compresses the spring individually, as the compression is a result of the distance between the two ends rather than the individual contributions of each force. Ultimately, the interaction between the wall and the person can be viewed as a cooperative effect in compressing the spring.