+ The Impulse-Momentum Theorem Learning Goal: To sam about the impulse-mamennum theorem and its applications in same common Usg the concept of momentum, Newton's second how can be rewnienas al where is the ner for F.. Acting on the object and is the case at which the object's momentum is changing (1) the object is observed during an intented of ame between imes 21 and 52, then imagration of both sides of equation (1) gives fFdt=fdt) The right side of equation (2) is simply the change in the objects momentum pi-Pi The left side is called the impulse of the not force and is denoted by J. Then equation (2) can be s J-Pi-Pi This equation is known as the impulso-mamonnum theorem. It states that the change in an objects momenrum is equal to the impulse of the net force acting on the object. In the Ass of a constant at tors Facting along the direction of motion, the impulsa momen theorem can be willen a Ft 1)-me my. (3) TF, as are the components of the coresponding vector quarring the chosen coordinate axts. If the motion in question is two dimensional it is often Figure 1 of 1 Let us now consider several two dimensional situations. A particia of mass m is moving in the positivax direction at speed. After a certain constant foros is applied to the partice, moves in the positive y direction ar spesid 2 Part E Find the magnitude of the impulse J delivered to the particle. Express your answer in terms of m and c. Use three significant figures in the numerical coefficient. J= Submit 01 Incorrect; Try Again; 2 attempts remaining Your awer eher corsan correct numerical mubpher or ts massing one 2 3 05 Part F Which of the vectors below best represents the direction of the impulse vector 7 (11-1) 07 OB | Submit 4 A O Part G ? Mint My Ass Give Up Renew Part Mr. Ama Cive U Incorrect; Try Again; 5 attempts remaining