질량중심 공식 x ˉ = ∫ C x ρ d s ∫ C ρ d s \bar x = \dfrac{\int_C x\rho\,\mathrm{d}s}{\int_C \rho\,\mathrm{d}s} x ˉ = ∫ C ρ d s ∫ C x ρ d s 등을 사용한다. 풀이 과정을 더 분명히 하기 위해 계산을 여러 단계로 나누어 진행한다.
x ( t ) = t + 1 2 t 2 x ′ ( t ) = 1 + t y ( t ) = t − 1 2 t 2 y ′ ( t ) = 1 − t z ( t ) = 4 3 t 3 / 2 z ′ ( t ) = 2 t \begin{aligned}
x(t)&= t+ \frac12 t^2 & x'(t)&=1+t\\
y(t)&= t- \frac12 t^2 & y'(t)&=1-t\\
z(t)&=\frac43 t^{3/2} & z'(t)&=2\sqrt{t}
\end{aligned} x ( t ) y ( t ) z ( t ) = t + 2 1 t 2 = t − 2 1 t 2 = 3 4 t 3/2 x ′ ( t ) y ′ ( t ) z ′ ( t ) = 1 + t = 1 − t = 2 t
x ′ ( t ) 2 + y ′ ( t ) 2 + z ′ ( t ) 2 = 1 + 2 t + t 2 + 1 − 2 t + t 2 + 4 t = 2 ( t 2 + 2 t + 1 ) = 2 ( t + 1 ) ρ ( x ( t ) , y ( t ) , z ( t ) ) = x ( t ) + y ( t ) 2 = ( t + t 2 / 2 ) + ( t − t 2 / 2 ) 2 = t \begin{aligned}
\sqrt{x'(t)^2+y'(t)^2+z'(t)^2}&=\sqrt{1+2t+t^2+1-2t+t^2+4t}=\sqrt{2(t^2+2t+1)}= \sqrt{2}(t+1)\\
\rho(x(t),y(t),z(t))&= \frac{x(t)+y(t)}{2}={\frac{(t+t^2/2 )+( t - t^2/2)}{2}}= t
\end{aligned} x ′ ( t ) 2 + y ′ ( t ) 2 + z ′ ( t ) 2 ρ ( x ( t ) , y ( t ) , z ( t )) = 1 + 2 t + t 2 + 1 − 2 t + t 2 + 4 t = 2 ( t 2 + 2 t + 1 ) = 2 ( t + 1 ) = 2 x ( t ) + y ( t ) = 2 ( t + t 2 /2 ) + ( t − t 2 /2 ) = t
∫ C r e d ρ d s = ∫ 0 4 t 2 ( t + 1 ) d t = 2 3 ⋅ 11 2 3 ∫ C x r e d ρ d s = ∫ 0 4 ( t + 1 2 t 2 ) t 2 ( t + 1 ) d t = 2 ∫ 0 2 2 ( t 4 2 + 3 2 t 3 + t 2 ) d t = 2 ( 2 9 5 + 3 ( 2 5 ) + 2 6 3 ) = 2 5 ⋅ 103 2 15 ∫ C y r e d ρ d s = ∫ 0 4 ( t − 1 2 t 2 ) t 2 ( t + 1 ) d t = 2 ∫ 0 2 2 ( − t 4 2 + t 3 2 + t 2 ) d t = 2 ( − 2 9 5 + 2 5 + 2 6 3 ) = − 2 5 ⋅ 23 2 15 ∫ C z r e d ρ d s = ∫ 0 4 ( 4 3 t 3 / 2 ) t 2 ( t + 1 ) d t = 4 2 3 ∫ 0 2 2 ( t 7 / 2 + t 5 / 2 ) d t = 4 2 3 ( 2 10 9 + 2 8 7 ) = 2 10 ⋅ 37 2 7 ⋅ 3 3 x ‾ = ∫ x ρ d s ∫ ρ d s = 2 5 ⋅ 103 2 15 2 3 ⋅ 11 2 3 = 412 55 ≈ 7.5 y ‾ = ∫ y ρ d s ∫ ρ d s = − 2 5 ⋅ 23 2 15 2 3 ⋅ 11 2 3 = − 92 55 ≈ − 1.7 z ‾ = ∫ z ρ d s ∫ ρ d s = 2 10 ⋅ 37 2 7 ⋅ 3 3 2 3 ⋅ 11 2 3 = 4736 693 ≈ 6.8 \begin{aligned}
\int_C {red}\rho \,\mathrm{d}s&=\int_0^4 t\, \sqrt{2}(t+1)\,\mathrm{d}t
=\frac{2^3\cdot 11\sqrt{2}}{3}\\
\int_C x {red}\rho \,\mathrm{d}s&=\int_0^4 \left(t+\frac12t^2\right) t\, \sqrt{2}(t+1)\,\mathrm{d}t
=\sqrt{2}\int_0^{2^2} \left(\frac{t^4}{2}+\frac{3}{2}t^3
+t^2\right)\ \mathrm{d}t\\
&=\sqrt{2}\left(\frac{2^9}{5} +3(2^5)+\frac{2^6}{3}\right)
=\frac{2^5\cdot103\sqrt 2}{15}\\
\int_C y {red}\rho \,\mathrm{d}s&=\int_0^4 \left(t-\frac12t^2\right) t\, \sqrt{2}(t+1)\,\mathrm{d}t=\sqrt2\int_0^{2^2}\left(-\frac{t^4}{2}+\frac{t^3}{2}+t^2 \right)\mathrm{d}t\\
&=\sqrt{2}\left(-\frac{2^9}{5}+{2^5}+\frac{2^6}{3} \right)
=-\frac{2^5\cdot 23\sqrt 2}{15}\\
\int_C z {red} \rho\, \mathrm{d}s&=\int_0^4 \left(\frac{4}{3}t^{3/2}\right) t\, \sqrt{2}(t+1)\,\mathrm{d}t=\frac{4\sqrt2}{3}\int_0^{2^2}
\left( t^{7/2}+t^{5/2}\right)\mathrm{d}t\\
&=\frac{4\sqrt2}{3}\left( \frac{2^{10}}{9}+\frac{2^8}{7}\right)=\frac{2^{10}\cdot37\sqrt{2}}{7\cdot 3^3}
\\
\overline{x}&=\frac{\int x \rho\,\mathrm{d}s}{\int \rho\,\mathrm{d}s}=\frac{\frac{2^5\cdot103\sqrt 2}{15}}{\frac{2^3\cdot 11\sqrt{2}}{3}}=\frac{412}{55}\approx 7.5\\
\overline{y}&=\frac{\int y \rho\,\mathrm{d}s}{\int \rho\,\mathrm{d}s}=\frac{-\frac{2^5\cdot 23\sqrt 2}{15}}{\frac{2^3\cdot 11\sqrt{2}}{3}}=-\frac{92}{55}\approx-1.7\\
\overline{z}&=\frac{\int z \rho\,\mathrm{d}s}{\int \rho\,\mathrm{d}s}=\frac{\frac{2^{10}\cdot37\sqrt{2}}{7\cdot 3^3}}{\frac{2^3\cdot 11\sqrt{2}}{3}}=\frac{4736}{693}\approx 6.8
\end{aligned} ∫ C re d ρ d s ∫ C x re d ρ d s ∫ C y re d ρ d s ∫ C z re d ρ d s x y z = ∫ 0 4 t 2 ( t + 1 ) d t = 3 2 3 ⋅ 11 2 = ∫ 0 4 ( t + 2 1 t 2 ) t 2 ( t + 1 ) d t = 2 ∫ 0 2 2 ( 2 t 4 + 2 3 t 3 + t 2 ) d t = 2 ( 5 2 9 + 3 ( 2 5 ) + 3 2 6 ) = 15 2 5 ⋅ 103 2 = ∫ 0 4 ( t − 2 1 t 2 ) t 2 ( t + 1 ) d t = 2 ∫ 0 2 2 ( − 2 t 4 + 2 t 3 + t 2 ) d t = 2 ( − 5 2 9 + 2 5 + 3 2 6 ) = − 15 2 5 ⋅ 23 2 = ∫ 0 4 ( 3 4 t 3/2 ) t 2 ( t + 1 ) d t = 3 4 2 ∫ 0 2 2 ( t 7/2 + t 5/2 ) d t = 3 4 2 ( 9 2 10 + 7 2 8 ) = 7 ⋅ 3 3 2 10 ⋅ 37 2 = ∫ ρ d s ∫ x ρ d s = 3 2 3 ⋅ 11 2 15 2 5 ⋅ 103 2 = 55 412 ≈ 7.5 = ∫ ρ d s ∫ y ρ d s = 3 2 3 ⋅ 11 2 − 15 2 5 ⋅ 23 2 = − 55 92 ≈ − 1.7 = ∫ ρ d s ∫ z ρ d s = 3 2 3 ⋅ 11 2 7 ⋅ 3 3 2 10 ⋅ 37 2 = 693 4736 ≈ 6.8
이렇게 긴 계산을 한 뒤에는 결과가 타당한지 검토해 보는 것이 좋다. 0 ≤ t ≤ 4 0 \le t \le 4 0 ≤ t ≤ 4 일 때, 철사는 다음 구간에 놓여 있다: 0 ≤ x ≤ 12 0 \le x \le 12 0 ≤ x ≤ 12 , − 4 ≤ y ≤ 1 / 2 -4 \le y \le 1/2 − 4 ≤ y ≤ 1/2 , 0 ≤ z ≤ 32 / 3 0 \le z \le 32/3 0 ≤ z ≤ 32/3 . 질량중심의 좌표는 모두 이 구간 안에 들어 있다. 이것이 답이 옳음을 보장하지는 않지만 좋은 징조이다. 예를 들어 x ‾ \overline x x 가 음수이거나 z ‾ \overline z z 가 11보다 컸다면, 무언가 잘못되었음을 알 수 있었을 것이다.