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The_Cambridge_Handbook_of_Physics_Formulas

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2.6 Mensuration<br />

39<br />

Curve measure<br />

Length <strong>of</strong> plane<br />

curve l =<br />

∫ b<br />

Surface <strong>of</strong><br />

revolution A =2π<br />

Volume <strong>of</strong><br />

revolution<br />

a<br />

V = π<br />

[<br />

1+<br />

∫ b<br />

a<br />

∫ b<br />

a<br />

y<br />

( ) ] 2 1/2<br />

dy<br />

dx (2.279)<br />

dx<br />

[<br />

1+<br />

a<br />

b<br />

y(x)<br />

l<br />

start point<br />

end point<br />

plane curve<br />

length<br />

( ) ] 2 1/2<br />

dy<br />

dx (2.280) A surface area<br />

dx<br />

y 2 dx (2.281) V volume<br />

[ ( ) ]<br />

Radius <strong>of</strong><br />

2 3/2 ( dy d 2 ) −1<br />

y<br />

curvature ρ = 1+<br />

dx dx 2 (2.282)<br />

ρ<br />

radius <strong>of</strong><br />

curvature<br />

2<br />

Differential geometry a<br />

Unit tangent<br />

Unit principal normal<br />

ˆτ = ṙ<br />

|ṙ| = ṙ<br />

v<br />

ˆn =<br />

¨r −˙v ˆτ<br />

|¨r −˙v ˆτ|<br />

τ tangent<br />

(2.283) r curve parameterised by r(t)<br />

v |ṙ(t)|<br />

(2.284) n principal normal<br />

Unit binormal ˆb = ˆτ ׈n (2.285) b binormal<br />

Curvature<br />

κ = |ṙרr|<br />

|ṙ| 3 (2.286) κ curvature<br />

Radius <strong>of</strong> curvature<br />

ρ = 1 κ<br />

(2.287) ρ radius <strong>of</strong> curvature<br />

Torsion<br />

λ = ṙ ·(¨r×... r )<br />

|ṙרr| 2 (2.288) λ torsion<br />

ˆn<br />

˙ˆτ = κvˆn (2.289)<br />

osculating<br />

plane<br />

Frenet’s formulas<br />

˙ˆn = −κv ˆτ +λvˆb (2.290)<br />

normal plane<br />

ˆτ<br />

˙ˆb = −λvˆn (2.291)<br />

ˆb<br />

r<br />

rectifying<br />

plane<br />

origin<br />

a For a continuous curve in three dimensions, traced by the position vector r(t).

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