Investigating the Newton's Laws of Motion

This lab primarily aims at investigating Newton’s laws of motion. It involves the experiment on mass, velocity, time, and the acceleration of a cart. The experimental values of acceleration are compared with those of the theoretical ones.


Theory


The lab involves experimenting with a cart that is self-propelled using a fan. Other procedures carried out include a cart on a horizontal and the one on include track, pulled by a rope attached to a mass that is hanging. Newton's laws of motion help in describing the effects of force on a motion of a system or object. In brief, the acceleration of a system occurs in a manner governed by the mass and the net force of the system if there is an imbalance of all the forces acting on the system. This experiment uses the acceleration of a cart for the examination of Newton's laws of motion.


Data


Tables 1: A Cart Self-Propelled by a Fan


Mass (kg)


Acceleration of cart (m/s2)


F = mass x acceleration of cart (N)


From v vs. t graph


From x vs. t graph


Average


0.518


0.303


0.153


0.228


0.118


0.997


0.155


0.078


0.117


0.117


Table 2: A Cart on Horizontal Track


Mass (Kg)


MASS (KG)


Acceleration of cart (m/s2)


T (N)


Experiment


Theory


% error


From v vs. t graph


From x vs. t graph


Average


0.532


0.01


0.206


0.109


0.158


0.003


5166


0.002


0.02


0.383


0.192


0.228


0.008


2750


0.004


1.04


0.01


0.106


0.052


0.079


0.0008


4775


0.0008


0.02


0.195


0.097


0.146


0.003


4766


0.003


Table 3: A Cart on an Inclined Track


Mass (Kg)


MASS (KG)


θ (degrees)


Sine θ


Acceleration of the cart (m/s2)


T (N)


Experiment


V vs. t graph


x vs. t graph


Average


Theory


% error


1.04


0.2


3.04


0.053


0.941


0.519


0.73


0.085


758.8


0.129


6.43


0.112


0.395


0.302


0.449


0.5


1396.6


0.084


9.38


0.163


0.197


0.047


0.147


0.004


3575


0.029


Sample Calculations


From table 1, it is apparent acceleration, α = varies inversely with mass (m). For example, a mass of 0.518 kg produces an average acceleration of 0.228 m/s2. Also, a mass of 0.997 kg has an acceleration of 0.117 m/s2.


Force, F = mα = 0.518 x 0.228 = 0.118 N.


For the second mass, F = 0.997 x 0.117 = 0.117 N.


The average value of force = 0.1175 N.


Graphs


Figure 1: Graph of Acceleration versus Sine θ


In this graph, R2 = 0.7949 and y = 7.5x – 0.37


Questions and Answers


Question 1


Figure 1: Free Body Diagram


If m = 1.04 kg and M = 0.2 kg, then sine θ = (100 – 30)/ 95 = 0.7


T = (1.04 x 0.2)/ (1.04 + 0.2) x 9.8 = 1.64 N


1.64 – (0.2 x 9.8 x 0.7) = 0.268 N


If T – mg x sine θ = and ma cart F, then the nominal force of the cart = 0.268 N


Equation (8), a = g [M-(m x sine θ)]/ [m + M]


= 9.8[0.2-1.04 x 0.7)]/ [1.04 + 0.2] = 5.1744/ 1.24 = 4.173


Equation (9), T = Mmg (1+ sine θ)/ (m + M)


= [(0.2 x 1.04 x 9.8)] x [(1 + 0.7)/ (1.04 + 0.2)] = 2.0384/ 1.37 = 1.488


Question 2


Figure 2: Schematic Diagrams


Question 3


The force of the cart F depends on its mass. The answers agree with the results in Table 1.


Question 4


In such a scenario, the hanging mass’ acceleration would be equal to that of gravity 9.8 m/s2


because of the free fall.


Question 5


The cart’s acceleration would be close to that of the gravity 9.8m/s2 due to the free fall on the frictionless ramp. The acceleration = angle of inclination would be = g x sine θ. 


Conclusion


This experiment helped in showing how a net force is produced by the forces acting on the cart. Even though the lab achieved it objective of investigating Newton's laws of motion, there were some significant errors in the experimental values.


Obstacles/ Errors


As can be seen in all the three tables, the percentage errors are quite significant. Lengthy calculations faultiness of the equipment might have resulted in these uncertainties.

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