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Newton’s Second Law AP  Physics 1 FRQ

Newton’s Second Law AP  Physics 1 FRQ – Exam Style Questions etc.

Newton’s Second Law AP  Physics 1 FRQ

Unit: 2. Force and Translational  Dynamics

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AP Physics 1 Exam Style Questions – All Topics

Exam Style Practice Questions, Newton's Second Law AP  Physics 1 FRQ

Question

A race car with a weight of \(1,709.94 \mathrm{~N}\) moves at a constant \(3.41 \mathrm{~m} / \mathrm{s}^{\wedge} 2\) while experiencing \(425.78 \mathrm{~N}\) worth of friction. What force must the engine be providing the car?

▶️Answer/Explanation

Ans:

\(\begin{aligned} & w=1709.94 \\ & a=3.41 \text { m/s^2 } \\ & \text { friction }=425.78 \mathrm{~N} \\ & \text { Force }- \text { Friction }=\mathrm{ma} \\ & \text { Force }-425.78=\left(\frac{w}{g}\right) a \\ & \text { Force }=425.78+\frac{1709.94}{9.8} \times 3.41 \\ & F=425.78+594.98 \\ & F=1020.77~N\end{aligned}\)

Question

A massless tray is placed on an inclined plane with an angle of incline of θ. There is a coefficient of static friction \(\mu _{s}\) between the inclined plane and the massless tray. The tray is attached to a box of mass M by the pulley system shown below.

(a) If mass can be loaded onto the massless tray, how much mass m has to be loaded to stop the tray from being pulled up the inclined plane by M?
(b) How much mass m has to be loaded until the tray starts sliding down the inclined plane?
(c) If \(\mu _{k}\) = 0.3 and θ = 45°, what is the acceleration of the massless tray if m = 4M?

▶️Answer/Explanation

Ans:

(a) The forces acting on the m mass are \(F _{T}\) (the tension in the string connecting it to M mass), \(F _{w}\) (the weight of the mass m), \(F _{N}\) (the normal force exerted by the inclined plane), and \(F _{f}\) (the force of static friction).

The forces acting on the M mass are \(F _{T}\) (the tension in the string connecting it to the m mass) and \(F _{w}\) (the weight of the block).

In order to stop the tray from moving, the net force on both the M mass and the mass m loaded on the tray must be zero. Newton’s First Law applied to the M mass yields

\(F_{w2}-F_{T}=0\Rightarrow F_{T}=F_{w2}=Mg\)

Newton’s First Law applied to the m yields

\(F_{T}-F_{g}-F_{f}=0\Rightarrow F_{T}-mg\sin (\theta)-\mu _{s}mg\cos (\theta )=0\)

Substituting \(F _{T}\) = Mg, you get

\(Mg-mg\sin \theta -\mu _{s}mg\cos \theta =0\)

\(mg\sin \theta +\mu _{s}mg\cos \theta =Mg\)

\(m=\frac{Mg}{g\sin \theta +\mu _{s}g\cos \theta}\)

(b) As the mass is trying to slide down the incline, the force of friction is acting in the opposite direction as in (a). There is no change to the M mass, so Newton’s First Law applied to the M mass still yields

\(F_{w2}-F_{T}=0\Rightarrow F_{T}=F_{w2}=Mg\)

Newton’s First Law applied to the m yields

\(F_{T}+F_{g}-F_{f}=0\Rightarrow F_{T}+mg\sin \theta -\mu _{s}mg\cos \theta =0\)

Substituting \(F _{T}\) = Mg, you get

\(Mg+mg\sin \theta -\mu _{s}mg\cos \theta =0\)

\(mg\sin \theta -\mu _{s}mg\cos \theta =Mg\)

\(m=\frac{Mg}{g\sin \theta +\mu _{s}g\cos \theta }\)

In order for the massless tray to start sliding down the inclined plane, m has to be greater than \(\frac{Mg}{g\sin \theta +\mu _{s}g\cos \theta }\).

(c) Newton’s First Law applied to the M mass yields

\(F_{T}-F_{w2}=Ma\Rightarrow F_{T}=F_{w2}+Ma\Rightarrow F_{T}=Mg+Ma\)

Newton’s First Law applied to the m yields

\(F_{g}-F_{f}-F_{T}=ma\Rightarrow mg\sin \theta -\mu _{k}mg\cos \theta -F_{T}=ma\)

Substituting \(F _{T}\) = Mg + Ma, you get

Plugging in m = 4M, θ = 45°, and\(\mu _{k}\) = 0.3, you get

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