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OpenStudy (anonymous):
I always like to tag ganeshie
ganeshie8 (ganeshie8):
lol ur tags always dread me.. :/
OpenStudy (jhannybean):
@ganeshie8 is too modest.
OpenStudy (anonymous):
Ok, so Let H be a solid hemisphere of radius a whose density at any point is proportional to its distance from the center of the base.
Find the mass H, there's more but just need the set up really
OpenStudy (anonymous):
So density = kp
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OpenStudy (jhannybean):
Eugh densities... doyou have to find the center of mass and stuff...
OpenStudy (anonymous):
yeah but w e lets just find mass
OpenStudy (anonymous):
Also asks for moment of inertia ahaha
OpenStudy (jhannybean):
Well, theres \(M_x\) and \(M_y\)
OpenStudy (jhannybean):
All I remember is that \(M_x\) has to do with y, and \(M_y\) has to do with x.
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ganeshie8 (ganeshie8):
mass = density * volume
OpenStudy (anonymous):
agree
OpenStudy (jhannybean):
You just apply the formula for both of those.
ganeshie8 (ganeshie8):
just setup a triple integral over H for the density
OpenStudy (anonymous):
p is from 0 to a then?
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OpenStudy (jhannybean):
Oh wait, from what ganeshie is saying..
OpenStudy (anonymous):
theta 0 to 2 pi
OpenStudy (anonymous):
phi though
OpenStudy (jhannybean):
\[M= \rho A = \rho(x,y)\cdot \Delta x \cdot \Delta y\]
ganeshie8 (ganeshie8):
should be easy after doing that previous hard problem..
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OpenStudy (jhannybean):
Right?
OpenStudy (jhannybean):
I remembered this because area across a solid volume is always with respect to both change in x and y.
OpenStudy (jhannybean):
\[M = \iint_R\rho(x,y)dxdy\]
ganeshie8 (ganeshie8):
that works for a solid without thickness..
we need to add another dimension for thickness...
OpenStudy (jhannybean):
Oh... haha, that'sz what I was missing.
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OpenStudy (jhannybean):
The `thickness` as in constant value \(k\).
OpenStudy (jhannybean):
\[M = \iint_Rk\rho(x,y)dxdy\]
ganeshie8 (ganeshie8):
\[M = \iint_R\rho(x,y,z)dxdydz\]
here \(\rho(x,y,z)\) is the density function.. not to be confused with distance from origin in spherical coordinates..