Physics Dynamics: Forces Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund 2012-2013 Department.

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Physics Dynamics: Forces Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund Department of Curriculum and Pedagogy FACULTY OF EDUCATION

Question Title Blocks on a Pyramid m2m2 m1m1 θ θ

Question Title A.m 1 g B.m 1 gsinθ C.m 1 gcosθ D.m 1 E.No idea A block is at rest on the rough surface of a pyramid. What is the normal force acting on the block if its mass is m 1 and the slope is θ degrees? Question Title Blocks on a Pyramid I m1m1 θ

Comments Answer: C Justification: From a free body diagram of the block (shown below), we see that the normal force must be equal to the y- component of the force due to gravity, in order to maintain a net force along the y-axis of 0. Comments Solution +x +y θ f m1gm1g N mg y mg x mg y is adjacent to the angle, so: mg y = m 1 gcosθ θ

Question Title A.m 1 g B.m 1 g(μcosθ - sinθ) C.m 1 g(sinθ + μcosθ) D.m 1 gsinθ E.No idea If the coefficient of friction is μ, what is the net force acting on the block? Question Title Blocks on a Pyramid II m1m1 θ +x +y

Comments Answer: B Justification: Using the free body diagram in the last question, we see that the force acting on the block is mostly contributed by the component of gravity parallel to the ramp (since the perpendicular component is cancelled by the normal force), which has a value of m 1 gsinθ. The normal force is m 1 gcosθ and the coefficient of friction is μ, giving a friction force of μm 1 gcosθ. The friction force and gravity force are in opposite directions, with the friction force pointing in the positive x direction. F net = m 1 g(μcosθ – sinθ) Notice, since the block is at rest, we are talking About static friction and μ s. Comments Solution +x +y θ f m1gm1g N mg y mg x θ

Question Title A.F g1x B.F g1 sinθ – F fric1 C.F g1 sinθ - F fric1 - F g2 + F fric2 D.F g1 sinθ – F fric1 – F g2 – F fric2 E.No idea Here we have the same situation except there are now two masses connected by a wire and a pulley. The angles and coefficients of friction are the same. If m 1 >m 2, what would be the net force on m 1 ? Question Title Blocks on a Pyramid III m2m2 m1m1 θ θ +x +y +x

Comments Answer: D Justification: The information m 1 >>m 2 means that the m 1 will go down the ramp while m 2 will go up the ramp. Thus, the forces on block 1 due to gravity and friction oppose each other, while the forces of gravity and friction on m 2 will be directed in the same direction. The forces on block 2 are in the same direction, because friction always opposes the direction of motion. The forces of tension T are the same on both blocks as they are connected by the same string. Comments Solution +x +y m2m2 m1m1 θ θ f1f1 Fg 1 f2f2 Fg 2 T T

Question Title A.m 1 g B.m 1 g(sinθ - μcosθ) C.m 1 g(sinθ - μcosθ) - m 2 g(sinθ - μcosθ) D.m 1 g(sinθ - μcosθ) - m 2 g(sinθ + μcosθ) E.No idea Here we have the same situation except there are now two masses connected by a wire and a pulley. The angles and coefficients of friction are the same. If m 1 >m 2, what would be the magnitude of the net force on m 1 ? Question Title Blocks on a Pyramid IV m2m2 m1m1 θ θ +x

Comments Answer: D Justification: The force going forward is m 1 gsinθ (gravity on m 1 ), while the three forces opposing it are μm 1 gcosθ (friction on m 1 ), m 2 gcosθ (gravity on m 2 ), and μm 2 gcosθ (friction on m 2 ). The signs in front of the three forces opposing the gravity on m 1 are all negative, but since m 2 is taken out of the brackets along with the negative sign in front of it, D is the correct answer. m 1 gsinθ - μm 1 gcosθ - m 2 gcosθ - μm 2 gcosθ = m 1 g(sinθ – μcosθ) - m 2 g(cosθ + μcosθ) Comments Solution +x +y m2m2 m1m1 θ θ f1f1 Fg 1 f2f2 Fg 2 T T

Question Title There are two masses connected by a wire and pulley resting on a pyramid. The angles and coefficients of friction are the same. If m 2 >m 1, what would be the magnitude of the net force on m 1 ? Question Title Blocks on a Pyramid V m2m2 m1m1 θ θ A.F g2 sinθ B.F g2 sinθ – F fric2 C.F g2 sinθ – F fric2 – F g1 + F fric1 D.F g2 sinθ – F fric2 – F g1 – F fric1 E.No idea

Comments Answer: D Justification: This is essentially the same question as number 3, except the roles of m 1 and m 2 are reversed. Friction always opposes The direction of the positive x- axis has also been reversed. Comments Solution m2m2 m1m1 θ θ +x

Question Title There are two masses connected by a wire and pulley resting on a pyramid. The angles and coefficients of friction are the same. What is the maximum value of that allows the masses to stay still? Question Title Blocks on a Pyramid VI m2m2 m1m1 θ θ

Comments Answer: C Justification: We only need to consider the case of m 2 >m 1 because it asks for the maximum value of The contraption will be at rest if the driving force is less than or equal to the opposing forces: m 2 gsinθ ≤ μm 1 gcosθ + m 1 gsinθ + μm 2 gcosθ. Regrouping, we find that this is true if m 2 (sinθ - μcosθ) ≤ m 1 (sinθ + μcosθ). Therefore, Comments Solution

Question Title There are two masses connected by a wire and pulley resting on a pyramid. The angles and coefficients of friction are the same. What is the minimum value of that allows the masses to stay still? Question Title Blocks on a Pyramid VII m2m2 m1m1 θ θ

Comments Answer: D Justification: This is simply a reversal of question 5, except this time m 1 is the “dominant” block. Because the system is symmetric, for m 1 >m 2, (reverse the roles of m 1 and m 2 in question 5). We then find the answer by simply taking the reciprocal (while noting the greater than sign reverses). Comments Solution