Rectus femoris
Muscles of the iliac and anterior femoral regions. (Rectus femoris highlighted in red.)
Details
Origin	anterior inferior iliac spine and the exterior surface of the bony ridge which forms the iliac portion of the acetabulum
Insertion	inserts into the patellar tendon as one of the four quadriceps muscles
Artery	lateral femoral circumflex artery
Nerve	femoral nerve
Actions	knee extension; hip flexion
Antagonist	Hamstring
Identifiers
TA98	A04.0.00.016
TA2	1989
FMA	74993
Anatomical terms of muscle [edit on Wikidata]

A pennate or pinnate muscle (also called a penniform muscle) is a type of skeletal muscle with fascicles that attach obliquely (in a slanting position) to its tendon. This type of muscle generally allows higher force production but a smaller range of motion.^[1][2] When a muscle contracts and shortens, the pennation angle increases.^[3]

Etymology

The term "pennate" comes from the Latin pinnātus (“feathered, winged”), from pinna (“feather, wing”).

Types of pennate muscle

In skeletal muscle tissue, 10-100 endomysium-sheathed muscle fibers are organized into perimysium-wrapped bundles known as fascicles. Each muscle is composed of a number of fascicles grouped together by a sleeve of connective tissue, known as an epimysium. In a pennate muscle, aponeuroses run along each side of the muscle and attach to the tendon. The fascicles attach to the aponeuroses and form an angle (the pennation angle) to the load axis of the muscle. If all the fascicles are on the same side of the tendon, the pennate muscle is called unipennate (Fig. 1A). Examples of this include certain muscles in the hand. If there are fascicles on both sides of the central tendon, the pennate muscle is called bipennate (Fig. 1B). The rectus femoris, a large muscle in the quadriceps, is typical. If the central tendon branches within a pennate muscle, the muscle is called multipennate (Fig. 1C), as seen in the deltoid muscle in the shoulder.

Consequences of pennate muscle architecture

Physiological cross sectional area (PCSA)

One advantage of pennate muscles is that more muscle fibers can be packed in parallel, thus allowing the muscle to produce more force, although the fiber angle to the direction of action means that the maximum force in that direction is somewhat less than the maximum force in the fiber direction.^[4][5] The muscle cross sectional area (blue line in figure 1, also known as anatomical cross section area, or ACSA) does not accurately represent the number of muscle fibers in the muscle. A better estimate is provided by the total area of the cross sections perpendicular to the muscle fibers (green lines in figure 1). This measure is known as the physiological cross sectional area (PCSA), and is commonly calculated and defined by the following formula (an alternative definition is provided in the main article):^[6][7][8]

${\displaystyle {\text{PCSA))=((\text{muscle volume)) \over {\text{fiber length))}=((\text{muscle mass)) \over {\rho \cdot {\text{fiber length)))),}$

where ρ is the density of the muscle:

${\displaystyle \rho =((\text{muscle mass)) \over {\text{muscle volume))}.}$

PCSA increases with pennation angle, and with muscle length. In a pennate muscle, PCSA is always larger than ACSA. In a non-pennate muscle, it coincides with ACSA.

Relationship between PCSA and muscle force

The total force exerted by the fibers along their oblique direction is proportional to PCSA. If the specific tension of the muscle fibers is known (force exerted by the fibers per unit of PCSA), it can be computed as follows:^[9]

${\displaystyle {\text{Total force))={\text{PCSA))\cdot {\text{Specific tension))}$

However, only a component of that force can be used to pull the tendon in the desired direction. This component, which is the true muscle force (also called tendon force^[8]), is exerted along the direction of action of the muscle:^[8]

${\displaystyle {\text{Muscle force))={\text{Total force))\cdot \cos \Phi }$

The other component, orthogonal to the direction of action of the muscle (Orthogonal force = Total force × sinΦ) is not exerted on the tendon, but simply squeezes the muscle, by pulling its aponeuroses toward each other.

Notice that, although it is practically convenient to compute PCSA based on volume or mass and fiber length, PCSA (and therefore the total fiber force, which is proportional to PCSA) is not proportional to muscle mass or fiber length alone. Namely, the maximum (tetanic) force of a muscle fiber simply depends on its thickness (cross-section area) and type. By no means it depends on its mass or length alone. For instance, when muscle mass increases due to physical development during childhood, this may be only due to an increase in length of the muscle fibers, with no change in fiber thickness (PCSA) or fiber type. In this case, an increase in mass does not produce an increase in force.

Lower velocity of shortening

In a pennate muscle, as a consequence of their arrangement, fibers are shorter than they would be if they ran from one end of the muscle to the other. This implies that each fiber is composed of a smaller number N of sarcomeres in series. Moreover, the larger the pennation angle is, the shorter are the fibers.

The speed at which a muscle fiber can shorten is partly determined by the length of the muscle fiber (i.e., by N). Thus, a muscle with a large pennation angle will contract more slowly than a similar muscle with a smaller pennation angle.

Architectural gear ratio

Architectural gear ratio, also called anatomical gear ratio, (AGR) is a feature of pennate muscle defined by the ratio between the longitudinal strain of the muscle and muscle fiber strain. It is sometimes also defined as the ratio between muscle-shortening velocity and fiber-shortening velocity:^[10]

AGR = ε_x/ε_f

where ε_x = longitudinal strain (or muscle-shortening velocity) and ε_f is fiber strain (or fiber-shortening velocity).^[10]

It was originally thought that the distance between aponeuroses did not change during the contraction of a pennate muscle,^[5] thus requiring the fibers to rotate as they shorten. However, recent work has shown this is false, and that the degree of fiber angle change varies under different loading conditions. This dynamic gearing automatically shifts in order to produce either maximal velocity under low loads or maximal force under high loads.^[10][11]