Reading graphs is a superpower in physics. When you look at a graph, you aren't just seeing lines and curves; you are looking at the hidden physical properties of an object. In this problem, we are given the gravitational field graphs of two solid spheres, and we need to find the ratio of their masses. Let's decode the visual data!
The Anatomy of the Graph
Look closely at the shape of the curves. For a uniform solid sphere, the gravitational field behaves differently inside and outside the sphere.
Inside the sphere (r<R), the field increases linearly with distance from the center: E=R3GMr. This is why both curves start as straight lines from the origin.
Outside the sphere (r>R), the sphere behaves like a point mass, and the field drops off according to the inverse-square law: E=r2GM.
The most crucial point on this graph is the peak. The peak represents the exact boundary of the sphere—its surface (r=R). At this point, the gravitational field is at its absolute maximum:
Extracting Data for Sphere 1
Let's focus on the first curve. The peak occurs at a radius R1=1 m, and the maximum field value there is E1=2.
We can plug these values directly into our surface field formula:
Solving this gives us a clean expression for the mass parameter of the first sphere:
Extracting Data for Sphere 2
Now, let's do the exact same thing for the second curve. The peak is located at R2=2 m, and the maximum field is E2=3.
Substituting these into the formula:
Since 22=4, we multiply both sides by 4 to isolate GM2:
The Final Ratio
We are asked to find the ratio of the masses, M2M1. Notice that we don't actually need the value of the universal gravitational constant G, because it will beautifully cancel out when we take the ratio!
Plugging in the values we just found:
Simplifying the fraction, we get our final answer:
By simply understanding that the peak of the graph corresponds to the surface of the sphere, a seemingly complex graphical problem turns into a straightforward substitution exercise. Always look for the peaks!