Tension by gravity
In physics, tension is the force on a string connecting two objects. Generally, the tension is calculated from both ends toward the center. When the length of the pendulum is ll, let’s consider the pendulum raised and released by an angle θmθm. The mass of the string is assumed to be zero.
The source of force to move the pendulum is gravity(= mgmg). This gravity can be divided into two forces:
- Tension by gravity, T = mg⋅cosθmg⋅cosθ
- The force to moves the pendulum = mg⋅sinθmg⋅sinθ (= Vector sum of ‘T’ and ‘mg’)

Centripetal force of pendulum
When the pendulum descends from the top, one more power is added. It is the centripetal force to maintain the rotational motion of the pendulum.
If the length is ll and the speed is vv, the centripetal force is:
F=mv2lF=mv2l
Like ‘tension by gravity,’ the centripetal force goes from the end to the center.
Total tension applied to the string
The total tension applied to the string can be calculated as follows.
Thetotaltension=Tensionbygravity+Centripetalforce=mg⋅cosθ+mv2lThetotaltension=Tensionbygravity+Centripetalforce=mg⋅cosθ+mv2l
Let’s make the above expression simple with an expression related to θθ.
Consider a pendulum with the highest amplitude θmθm, and the current amplitude θθ.

The increased kinetic energy is equal to the reduced potential energy by the law of conservation of energy.
12mv2=mgl(cosθ–cosθm)∴v2=2gl(cosθ–cosθm)
Substituting the above equation into the total tension, we get:
Thetotaltension=Tensionbygravity+Centripetalforce=mg⋅cosθ+m⋅2gl(cosθ–cosθm)l=mg⋅cosθ+2mg(cosθ–cosθm)=mg(3cosθ–2cosθm)