moment of inertia of solid cylinder in its own axis derivation and mathematically
Answers
Explanation:
. We will use the general equation of moment of inertia:
dI = r2 dm
Now we move on to finding the dm. It is normally given as;
dm = ρ dV
In this case, the mass element can be expressed in terms of an infinitesimal radial thickness dr by;
dm = 2r L dr
In order to obtain dm we have to calculate dv first. It is given as;
dV = dA L
Meanwhile, dA is the area of the big ring (radius: r + dr) minus the smaller ring (radius: r). Hence;
dA = \pi (r + dr)^{2} – \pi r^{2}dA=π(r+dr)
2
–πr
2
dA = \pi (r + 2rdr + (dr)^{2}) – \pi r^{2}dA=π(r+2rdr+(dr)
2
)–πr
2
Notably, here the (dr)2 = 0.
dA = 2\pi r drdA=2πrdr
Answer:
Explanation:
1. We will use the general equation of moment of inertia:
dI = r² dm
Now we move on to finding the dm. It is normally given as;
dm = ρ dV
In this case, the mass element can be expressed in terms of an infinitesimal radial thickness dr by;
dm = 2r L dr
In order to obtain dm we have to calculate dv first. It is given as;
dV = dA L
Meanwhile, dA is the area of the big ring (radius: r + dr) minus the smaller ring (radius: r). Hence;
dA = π ( r+dr )² - πr² => dA = π (r + 2r dr + (dr)² ) - πr²
Notably, here the (dr)² = 0.
dA = 2πrdr
2. Substitution of dA into dV we get;
dV = 2πLdr
Now, we substitute dV into dm and we will have;
dm = 2πLdr
The dm expression is further substituted into the dI equation and we get;
dl = 2πr³Ldr
3. Alternatively, we have to find the expression for density as well. We use the equation;
p = M/V
Now,
p = M/πR²L
4. The final step involves using integration to find the moment of inertia of the solid cylinder. The integration basically takes the form of a polynomial integral form.
I = 2PπrL ₙ∫ᵇ r³dr => I = 2PπL r⁴/4 => I = 2π[m/πR²L] LR⁴/4.
Therefore, I = 1/2 MR²