Let
Ω
⊆
R
m
\Omega \subseteq {\mathbb {R}^m}
be a bounded open set,
∂
Ω
\partial \Omega
its boundary and
Δ
\Delta
the Laplacian on
R
m
{\mathbb {R}^m}
. Consider the elliptic differential equation: (1)
\[
−
Δ
u
=
λ
u
in
Ω
;
u
=
0
on
∂
Ω
.
- \Delta u = \lambda u\quad {\text {in}}\;\Omega ;\qquad u = 0\quad {\text {on}}\;\partial \Omega .
\]
It is known that the eigenvalues,
λ
i
{\lambda _i}
, of (1) satisfy (2)
\[
∑
i
=
1
n
λ
i
λ
n
+
1
−
λ
i
⩾
m
n
4
\sum \limits _{i = 1}^n {\frac {{{\lambda _i}}} {{{\lambda _{n + 1}} - {\lambda _i}}}} \geqslant \frac {{mn}} {4}
\]
provided that
λ
n
+
1
>
λ
n
{\lambda _{n + 1}} > {\lambda _n}
. In this paper we abstract the method used by Hile and Protter [2] to establish (2) and apply the method to a variety of second-order elliptic problems, in particular, to all constant coefficient problems. We then consider a variety of higher-order problems and establish an extension of (2) for problem (1) where the Laplacian is replaced by a more general operator in a Hilbert space.