Answer:
the sphere
Step-by-step explanation:
From the given information,
A free flow body diagrammatic expression for the small uniform disk and a small uniform sphere which are released simultaneously at the top of a high inclined plane can be seen in the image attached below.
From the diagram;
The Normal force mgsinθ - Friction force F = mass m × acceleration a
Meanwhile; the frictional force
![F = (I \alpha )/(R)](https://img.qammunity.org/2021/formulas/physics/college/x22nwk09ag8gn20lrk62xeznnmf7b655oq.png)
where
in a rolling motion
Then;
![F = (I a )/(R^2)](https://img.qammunity.org/2021/formulas/physics/college/ph3db8358h9u9hrtm4r6wb6b0343vjrtrq.png)
∴
The Normal force mgsinθ - F = m × a can be re-written as:
![\mathtt{mg sin \ \theta- (Ia)/(R^2) = ma}](https://img.qammunity.org/2021/formulas/physics/college/1k65luqblnjjh1a1yrmein8dyusrtozkqr.png)
making a the subject of the formula, we have:
![a = ((mg \ sin \theta)/(m + (I)/(R^2)))](https://img.qammunity.org/2021/formulas/physics/college/v3r9wutisj0uf1fsq5m2zv4dh9jq6vmrcm.png)
Similarly;
I = mk² in which k is the radius of gyration
∴
replacing I = mk² into the above equation , we have:
![a = ((mg \ sin \theta)/(m + (mk^2)/(R^2)))](https://img.qammunity.org/2021/formulas/physics/college/gyquhnwa00uj7qkibplkcb5ypcm5t0wotb.png)
where;
the uniform disk
the uniform sphere
∴
![a = (2)/(3) \ g sin \theta \ for \ the \ uniform \ disk](https://img.qammunity.org/2021/formulas/physics/college/m628e047ddb2ezjt1t4jmk9sjesgfjio8t.png)
![a = (5)/(7) \ g sin \theta \ for \ the \ uniform \ sphere](https://img.qammunity.org/2021/formulas/physics/college/kr4htechgohqenllf6j8nuacavvckxfzdz.png)
We can now see that the uniform sphere is greater than the disk as such the sphere will reach the bottom first.