| Now | y x | = | r h | where | y = r ( 1 cos θ ) |
| \ | x = | h r | r ( 1 cos θ ) | and | dx = h sin θ dθ |
| So | V = | &int0π/2 | ( r2 θ ½ r2 sin 2 θ ) h sin θ dθ |
| = | r2 h | &int0π/2 | ( θ ½ sin 2 θ ) sin θ dθ |
| &int0π/2 | θ sin θ dθ | = | [ θ cos θ ]0π/2 | | &int0π/2 | cos θ dθ | = | 1 |
| &int0π/2 | ( ½ sin 2 θ ) sin θ dθ | = | ¼ | &int0π/2 | ( cos 3 θ cos θ ) dθ |
| = | ¼ [ 13 sin 3θ sin θ ]0π/2 | = | 13 |
| So | V = | r2 h ( 1 13 ) | = | 23 r2 h |